ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation...

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D:\EMAG\2016-04-50/VOL13\F5.VFT—12PPS/P Modulation Techniques for Li⁃Fi Modulation Techniques for Li⁃Fi Mohamed Sufyan Islim and Harald Haas Li⁃Fi Research and Development Centre, Institute for Digital Communications, University of Edinburgh, Edinburgh EH9 3JL, UKAbstract Modulation techniques for light fidelity (Li⁃Fi) are reviewed in this paper. Li⁃Fi is the fully networked solution for multiple users that combines communication and illumination simultaneously. Light emitting diodes (LEDs) are used in Li ⁃ Fi as visible light transmitters, therefore, only intensity modulated direct detected modulation techniques can be achieved. Single carrier modulation techniques are straightforward to be used in Li⁃Fi, however, computationally complex equalization processes are required in fre⁃ quency selective Li⁃Fi channels. On the other hand, multicarrier modulation techniques offer a viable solution for Li⁃Fi in terms of power, spectral and computational efficiency. In particular, orthogonal frequency division multiplexing (OFDM) based modula⁃ tion techniques offer a practical solution for Li⁃Fi, especially when direct current (DC) wander, and adaptive bit and power load⁃ ing techniques are considered. Li ⁃ Fi modulation techniques need to also satisfy illumination requirements. Flickering avoidance and dimming control are considered in the variant modulation techniques presented. This paper surveys the suitable modulation techniques for Li⁃Fi including those which explore time, frequency and colour domains. light fidelity (Li⁃Fi); optical wireless communications (OWC); visible light communication (VLC); intensity modulation and direct detection (IM/DD); orthogonal frequency division multiplexing (OFDM) Keywords DOI: 10.3969/j. issn. 16735188. 2016. 02. 004 http://www.cnki.net/kcms/detail/34.1294.TN.20160413.1658.002.html, published online April 13, 2016 Special Topic This work is support by the UK Engineering and Physical Sciences Research Council (EPSRC) under Grants EP/K008757/1 and EP/M506515/1. April 2016 Vol.14 No.2 ZTE COMMUNICATIONS ZTE COMMUNICATIONS 29 1 Introduction ore than half a billion new communication de⁃ vices were added to the network services in 2015. Globally, mobile data traffic is predict⁃ ed to reach 30.6 exabytes per month by 2020 (the equivalent of 7641 million DVDs each month), up from 3.7 exabytes per month in 2015 [1]. The radio frequency band⁃ width currently used is a very limited resource. The increasing dependency on cloud services for storage and processing means that new access technologies are necessary to allow this huge increase in network utilization. The visible light spectrum on the other hand offers a 10,000 times larger unlicensed fre⁃ quency bandwidth that could accommodate this expansion of network capacity. Visible light communication (VLC) is the point⁃to⁃point high speed communication and illumination sys⁃ tem. Light fidelity (Li⁃Fi) is the complete wireless, bi⁃direction⁃ al, multi ⁃ user network solution for visible light communica⁃ tions that would operate seamlessly alongside other Long Term Evolution (LTE) and wireless fidelity (Wi⁃Fi) access technolo⁃ gies [2]. Li ⁃ Fi is a green communication method as it reuses the existing lightning infrastructure for communications. Infor⁃ mation is transmitted by the rapid subtle changes of light inten⁃ sity that is unnoticeable by the human eye. Recent studies have demonstrated data rates of 14 Gbps for Li⁃Fi using three off⁃the⁃shelf laser diodes (red, green and blue) [3]. It was also predict that a data rate of 100 Gbps is achievable for Li ⁃ Fi when the whole visible spectrum is utilized [3]. Li⁃Fi offers in⁃ herent security, and also it can be employed in areas where sensitive electronic devices are present, such as in hospitals. In addition, Li ⁃ Fi is a potential candidate for other applica⁃ tions such as underwater communications, intelligent transpor⁃ tation systems, indoor positioning, and the Internet of Things (IoT) [2]. Modulation techniques developed for intensity modulation and direct detection (IM/DD) optical wireless communication (OWC) systems are suitable for Li⁃Fi communications systems. However, these modulation techniques may not be suitable for all lightning regimes. Li⁃Fi transceivers are illumination devic⁃ es enabled for data communications. Therefore adapting IM/ DD modulation technique should first satisfy certain illumina⁃ tion requirements before being Li ⁃ Fi enabled. For example, modulation techniques should support dimmable illumination so that communication would be still available when the illumi⁃ nation is not required. Li⁃Fi uses off⁃the⁃shelf light emitting di⁃ odes (LEDs) and photodiodes (PDs) as channel front⁃end devic⁃ es. This restricts signals propagating throughout the channel to M 1

Transcript of ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation...

Page 1: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

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Modulation Techniques for LiFiModulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas(LiFi Research and Development Centre Institute for Digital Communications University of Edinburgh Edinburgh EH9 3JL UK)

Abstract

Modulation techniques for light fidelity (LiFi) are reviewed in this paper LiFi is the fully networked solution for multiple usersthat combines communication and illumination simultaneously Light emitting diodes (LEDs) are used in Li Fi as visible lighttransmitters therefore only intensity modulated direct detected modulation techniques can be achieved Single carrier modulationtechniques are straightforward to be used in LiFi however computationally complex equalization processes are required in frequency selective LiFi channels On the other hand multicarrier modulation techniques offer a viable solution for LiFi in termsof power spectral and computational efficiency In particular orthogonal frequency division multiplexing (OFDM) based modulation techniques offer a practical solution for LiFi especially when direct current (DC) wander and adaptive bit and power loading techniques are considered LiFi modulation techniques need to also satisfy illumination requirements Flickering avoidanceand dimming control are considered in the variant modulation techniques presented This paper surveys the suitable modulationtechniques for LiFi including those which explore time frequency and colour domains

light fidelity (LiFi) optical wireless communications (OWC) visible light communication (VLC) intensity modulation and directdetection (IMDD) orthogonal frequency division multiplexing (OFDM)

Keywords

DOI 103969j issn 167310490205188 2016 02 004httpwwwcnkinetkcmsdetail341294TN201604131658002html published online April 13 2016

Special Topic

This work is support by the UK Engineering and Physical SciencesResearch Council (EPSRC) under Grants EPK0087571 and EPM5065151

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 29

1 Introductionore than half a billion new communication devices were added to the network services in2015 Globally mobile data traffic is predicted to reach 306 exabytes per month by 2020

(the equivalent of 7641 million DVDs each month) up from37 exabytes per month in 2015 [1] The radio frequency bandwidth currently used is a very limited resource The increasingdependency on cloud services for storage and processingmeans that new access technologies are necessary to allow thishuge increase in network utilization The visible light spectrumon the other hand offers a 10000 times larger unlicensed frequency bandwidth that could accommodate this expansion ofnetwork capacity Visible light communication (VLC) is thepointtopoint high speed communication and illumination system Light fidelity (LiFi) is the complete wireless bidirectional multi user network solution for visible light communications that would operate seamlessly alongside other Long TermEvolution (LTE) and wireless fidelity (WiFi) access technologies [2] Li Fi is a green communication method as it reusesthe existing lightning infrastructure for communications Infor

mation is transmitted by the rapid subtle changes of light intensity that is unnoticeable by the human eye Recent studieshave demonstrated data rates of 14 Gbps for LiFi using threeofftheshelf laser diodes (red green and blue) [3] It was alsopredict that a data rate of 100 Gbps is achievable for Li Fiwhen the whole visible spectrum is utilized [3] LiFi offers inherent security and also it can be employed in areas wheresensitive electronic devices are present such as in hospitalsIn addition Li Fi is a potential candidate for other applications such as underwater communications intelligent transportation systems indoor positioning and the Internet of Things(IoT) [2]

Modulation techniques developed for intensity modulationand direct detection (IMDD) optical wireless communication(OWC) systems are suitable for LiFi communications systemsHowever these modulation techniques may not be suitable forall lightning regimes LiFi transceivers are illumination devices enabled for data communications Therefore adapting IMDD modulation technique should first satisfy certain illumination requirements before being Li Fi enabled For examplemodulation techniques should support dimmable illuminationso that communication would be still available when the illumination is not required LiFi uses offtheshelf light emitting diodes (LEDs) and photodiodes (PDs) as channel frontend devices This restricts signals propagating throughout the channel to

M

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Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

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strictly positive signals Single carrier modulation (SCM) techniques are straight forward to implement in LiFi Modulationtechniques such as onoff keying (OOK) pulseposition modulation (PPM) and M ary pulse amplitude modulation (M PAM) can be easily implemented However due to the dispersive nature of optical wireless channels such schemes requirecomplex equalizers at the receiver Therefore the performanceof these schemes degrades as their spectral efficiency (SE) increases On the other hand multiple carrier modulation (MCM)techniques such as the orthogonal frequency division multiplexing (OFDM) have been shown to be potential candidatesfor optical wireless channels since they only require single tapequalizer at the receiver Adaptive bit and power loading canmaximize the achievable data rates of OFDMbased LiFi systems by adapting the system loading to the channel frequencyresponse Moreover the DC wander and low frequency interference can be easily avoided in OFDM by optimizing the adaptive bitpower loading to avoid the low frequency subcarriersColour modulation techniques are unique to LiFi communication systems as the information is modulated on the instantaneous colour changes The colour dimension adds a new degree of freedom to LiFi The various modulation LiFi modulation techniques discussed in this paper are shown in Fig 1

This paper is organized as follows The main challenges forLi Fi modulation techniques are summarized in Section 2SCM techniques for Li Fi are detailed in Section 3 OFDMbased modulation techniques for LiFi are discussed in detailsin Section 4 including inherent unipolar OFDM techniqueshybrid OFDM modulation techniques and superpositionOFDM modulation techniques Other MCM techniques are revised in Section 5 The unique colour domain modulation techniques are discussed in Section 6 Finally the conclusion ispresented in Section 7 The paper is limited to single input single output (SISO) LiFi communication systems The spacedimension of LiFi is not considered in this paper

2 LiFi Modulation Techniques ChallengesLi Fi is an emerging high speed low cost solution to the

scarcity of the radio frequency (RF) spectrum therefore it is expected to be realized using the widely deployed off the shelfoptoelectronic LEDs Due to the mass production of these inexpensive devices they lack accurate characterizations In LiFilight is modulated on the subtle changes of the light intensitytherefore the communication link would be affected by the nonlinearity of the voltageluminance characteristic As a solution

ACOOFDM asymmetrically clipped optical OFDMADOOFDM asymmetrically clipped DC biased optical OFDM

ASCOOFDM asymmetrically and symmetricallyclipped optical OFDM

CAP carrierless amplitude modulationCIM colour intensity modulationCSK colour shift keying

DCOOFDM DC biased OFDMDFTsOFDM discrete Fourier transformation spread OFDM

DHT discrete Hartley transformeACOOFDM enhanced ACOOFDM

ePAMDMT enhanced PAMDMTeUOFDM enhanced unipolar OFDM

HACOOFDM hybrid asymmetrically clippedoptical OFDM

HCM Hadamard coded modulationLACOOFDM layered ACOOFDM

LiFi light fidelityMCM multicarrier modulationMM metameric modulation

MPAM Mary pulse amplitude modulationMPPM Mary pulse position modulation

OFDM orthogonal frequency modulationOOK onoff keying

PAMDMT pulse amplitude modulation discrete multitonePMOFDM position modulation OFDMPOFDM polar OFDM

PWM pulse width modulationRPOOFDM reverse polarity optical OFDM

SCM single carrier modulationSEEOFDM spectrally and energy efficient OFDMSFOOFDM spectrally factorized optical OFDM

WPDM wavelet packet division multiplexingFigure 1 LiFi modulation techniques considered in this paper

LiFi modulation tech

SCM

OOK

PWM

MPAM

MPPM

DFTsOFDM

CAP

DCOOFDM InherentunipolarACOOFDM

PAMDMT

UOFDM

SuperpositionOFDMeUOFDM

eACOOFDM

ePAMDMT

SEEOFDM

LACOOFDM

Hybrid

RPOOFDM

POFDM

SpatialOFDM

ASCOOFDM

SFOOFDM

PMOFDM

ADOOFDM

HACOOFDM

Other MCM

HCM

WPDM

DHT

Colour domainMod

CSK

CIM

MM

OFDM (MCM)

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predistortion techniques were proposed to mitigate nonlineardistortion [4] However as the LED temperature increases thevoltageluminance (VL) characteristic experiences memoryeffects Therefore the LED non linearity mitigation is still anopen research problem The limited bandwidth of LiFi communication channel leads to inter symbol interference (ISI) athigh data rates The LED frequency response is modeled as alowpass filter and it is the major contributor to the frequencyselectivity of Li Fi channels The modulation bandwidth overwhich the frequency response of most commercially availableLEDs can be considered flat is around 2-20 MHz [5] [6] However the usable bandwidth in LiFi could be extended beyondthe 3 dB cutoff frequency

Therefore modulation techniques with higher spectral efficiencies are key elements in a LiFi system design Satisfyingthe illumination requirements is a key element in LiFi Mostof the research on modulation techniques has been on the communication system performance of Li Fi system Factors suchas dimming illumination level control and flickering havebeen analyzed as secondary parameters of a LiFi system TheLiFi systems should be also considered as an illumination system with communications capability not the reverse

3 Single Carrier Modulation TechniquesSingle carrier modulation techniques were first proposed for

IMDD optical wireless communications based on infrared communications [7] Modulation techniques such as OOK pulseamplitude modulation (PAM) pulse width modulation (PWM)and PPM are straightforward to implement for Li Fi systemsIn general single carrier modulation techniques are suitablecandidates for LiFi when lowtomoderate data rates applications are required By switching the LED betweenldquoonrdquoandldquooffrdquostates the incoming bits can be modulated into the lightintensity Illumination control can be supported by adjustingthe light intensities of theldquoonrdquoandldquooffrdquostates without affecting the system performance Compensation symbols are proposed in the visible light communications standard IEEE802157 [8] to facilitate the illumination control at the expense of reducing the SE If the link budget offers high signalto noise ratios (SNR) MPAM can be used to modulate the incoming bits on the amplitude of the optical pulse [9]The position of the optical pulse is modulated into shorter durationchips in PPM with a position index that varies depending onthe incoming bits The PPM is more power efficient than OOKhowever it requires more bandwidth than OOK to supportequivalent data rates Differential PPM (DPPM) was proposedto achieve power andor SE gains [10] however the effect of unequal bit duration for the different incoming symbols could affect the illumination performance A solution was proposed in[11] to ensure that the duty cycle is similar among the differentsymbols to prevent any possible flickering Variable PPM(VPPM) was proposed in the VLC standard IEEE 802157 to

support dimming for the PPM technique and prevent any possible flickering The pulse dimming in VPPM is controlled bythe width of the pulse rather than the pulse amplitude Therefore VPPM can be considered as a combination of PPM andPWM techniques Multiple PPM (MPPM) was proposed [12] asa solution to the dimming capability of PPM where it was reported that it achieves higher spectral efficiencies than VPPMwith less optical power dissipation The advantages of PAMand PPM are combined in pulse amplitude and position modulation (PAPM) [13]

The performance comparison between single carrier andmulticarrier modulation techniques was studied in [14]- [18]for different scenarios and considerations The results may differ depending on the major considerations and assumptions ofeach study However in general the performance of single carrier modulation techniques deteriorate as the data rates increase due to the increased ISI Equalization techniques suchas optimum maximum likelihood sequence detection (MLSD)frequency domain equalizers (FDE) nonlinear decision feedback equalizers (DFE) and linear feed forward equalizer(FFE) are suitable candidates for equalization processes withdifferent degrees of performance and computational complexity[7] [19] [20] The single carrier frequency domain equalizer(SCFDE) was proposed for OWC as a solution to the high peakto average power ratio (PAPR) of OFDM in [12] [21] PPM SCFDE was considered in [22] and OOKSCFDE was considered in [23] The performance of OOK with minimum meansquare error equalization (MMSE) was compared with the performance of asymmetrically clipped optical (ACO)OFDM andthe performance of complex modulation Mary quadrature amplitude modulation (MQAM) ACOSCFDE in [18] It was reported that the performance of ACOSCFDE outperforms asymmetrically clipped optical OFDM (ACO OFDM) and OOK MMSE due to the high PAPR of ACOOFDM when the nonlinear characteristics of the LED are considered The performance of PAMSCFDE is compared with OFDM in [12] without consideration of the LED nonlinearity It was shown thatPAM SCFDE achieves higher performance gains when compared with OFDM at spectral efficiencies less than 3 bitssHz

Discrete Fourier transformation spread (DFTs) OFDM wasalso considered for LiFi as a SCM that has the benefits of anOFDM multicarrier system with lower PAPR [24] An extrapair of DFT and inverse discrete Fourier transformation (IDFT)operations are required to achieve DFTs OFDM Multiple independent streams of DFTs OFDM modulated waveforms areseparately transmitted through multiple LEDs in a single arrayThe performance of DFTs OFDM is reported to be better whencompared with DC biased optical OFDM (DCO OFDM) interms of both PAPR and bit error rate (BER) [24] A novel carrierless amplitude and phase (CAP) modulation was proposedfor Li Fi in [25] In order for CAP to suit the frequency response of LEDs the spectrum of CAP was divided into m subcarriers by the aid of finite impulse response (FIR) filter Al

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though CAP is computationally complex it could offer highspectral efficiencies in bandlimited LiFi channel

4 Optical OFDMSingle carrier modulation techniques require a complex

equalization process when employed at high data rates In addition effects such as DC wandering and flickering interferenceof florescent lights may influence the system performance atthe lower frequency regions of the used bandwidth On the other hand multicarrier modulation techniques such as OFDMcan convert the frequency selective fading of the communication channel into a flat fading by employing the computationally efficient single tap equalizer In addition OFDM supportsadaptive power and bit loading which can adapt the channelutilization to the frequency response of the channel This canmaximize the system performance Supporting multiuser communication systems is an inherent advantage of OFDM whereeach user could be allocated certain subcarriers At the OFDMtransmitter the incoming bits are modulated into specific modulation formats such as M QAM The M QAM symbols areloaded afterwards into orthogonal subcarriers with subcarrierspacing equal to multiple of the symbol duration The parallelsymbols can then be multiplexed into a serial time domain output generally using inverse fast Fourier transformation (IFFT)The physical link of LiFi is achieved using offtheshelf optoelectronic devices such as LED and photodetectors (PD) Dueto the fact that these light sources produce an incoherent lightthe OFDM timedomain waveforms are used in LiFi to modulate the intensity of the LED source Therefore these waveforms are required to be both unipolar and real valued

Hermitian symmetry is generally imposed on the OFDM input frame to enforce the OFDM time domain signal output intothe real domain Different variants of optical OFDM were proposed to achieve a unipolar OFDM output DC bias is used inthe widely deployed DCOOFDM [26] to realize a unipolar timedomain OFDM output However OFDM signals have a highPAPR which makes it practically impossible to convert all ofthe signal samples into unipolar ones The OFDM timedomainwaveform can be approximated with a Normal distributionwhen the length of the input frame is greater than 64 The DCbias point would be dependent on the VL characteristic of theLED Zero level clipping of the remaining negative samples after the biasing would result in a clipping distortion that coulddeteriorate the system performance High DC bias would alsoincur some distortion as a result of the upper clipping of theOFDM waveform due to the V L characteristic of the idealLED The forward output current characteristic of an LED isshown in Fig 2 Predistortion is used to linearize the dynamicrange of the LED The LED input and output probability distribution function (PDF) of the OFDM modulation signal are alsoshown The dynamic range of the LED is between the turnonbias and the maximum allowed current points of the LED The

input signal is biased and the output signal is clipped for values outside the dynamic range The optimization of the DC biasing point was studied in [27]- [29] The additional dissipation of electrical power in DCOOFDM compared with bipolarOFDM increases as the modulation order increases This leadsto electrical and optical power inefficiency when DCOOFDMis used with high M QAM modulation orders Illumination isan essential part of VLC therefore the DCO OFDM opticalpower inefficiency can be justified for some VLC applicationsHowever when energy efficiency is required an alternativemodulation approach is required41 Inherent Unipolar Optical OFDM Techniques

Unipolar OFDM modulation schemes were mainly introduced to provide energy efficient optical OFDM alternatives toDCOOFDM These schemes include ACOOFDM [30] pulseamplitude modulated discrete multitone modulation (PAM DMT) [31] flipped OFDM (FlipOFDM) [32] and unipolar orthogonal frequency division multiplexing (UOFDM) [33] Theyexploit the OFDM inputoutput frame structure to produce aunipolar time domain waveform output However all of theseschemes have a reduced SE compared with DCOOFDM due tothe restrictions imposed on their frame structures In this section ACOOFDM PAMDMT and UOFDMFlipOFDM modulation schemes are discussed411 ACOOFDM

A real unipolar OFDM waveform can be achieved by exploiting the Fourier transformation properties on the frequency domain input OFDM frames The principle of ACOOFDM [30] isto skip the even subcarriers of an OFDM frame by only loading the odd subcarriers with useful information (Fig 3) Thiscreates a symmetry in the time domain OFDM signal which al

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

LED light emitting diode PDF probability distribution functionFigure 2 The forwardoutput current characteristic of an LED

I f

I out

LED transfer function

After predistortion

Dynamic rangeInput PDF

Output PDF

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lows the distortionless clipping of the negative samples without the need of any DC biasing (Fig 4) Clipping of the negative values is distortionless since all of the distortion will onlyaffect the evenindexed subcarriers However skipping half ofthe subcarriers reduces the SE of ACOOFDM to half of that inDCOOFDM A penalty of 3 dB should applied to the signaltonoise ratio (SNR) of ACOOFDM when compared with bipolarOFDM since half of the signal power is lost due to clippingHermitian symmetry is also used to guarantee a real valuedACOOFDM output At the receiver after a fast Fourier transformation (FFT) is applied on the incoming frame only oddsubcarriers are considered412 PAMDMT

A real unipolar optical OFDM is realized in PAMDMT byexploiting the Fourier properties of imaginary signals The realcomponent of the subcarriers is not used in PAMDMT whichrestricts the modulation scheme used to MPAM (Fig 3) Byonly loading MPAM modulated symbols on the imaginary components of the subcarriers an antisymmetry in the time domain waveform of PAMDMT would be achieved (Fig 5) Thiswould facilitate the distortionless zero level clipping of PAMDMT waveform as all of the distortion would only affect the re

al component of the subcarriers Hermitian symmetry is alsoused to guarantee a real valued PAMDMT output PAMDMTis more attractive than ACO OFDM when bit loading techniques are considered as the PAMDMT performance can beoptimally adapted to the frequency response of the channelsince all of the subcarriers are used The SE of PAMDMT issimilar to that of DCOOFDM PAMDMT has a 3 dB fixedpenalty when compared with bipolar OFDM at an appropriateconstellation size as half of the power is also lost due to clipping At the receiver the imaginary part of the subcarriers isonly considered while the real part is ignored413 UOFDMFlipOFDM

The concept and performance of UOFDM and FlipOFDMis identical In this paper the term UOFDM is used howeverall discussion and analysis is applicable to both schemes Hermitian symmetry is applied on the incoming frame of MQAMsymbols The bipolar OFDM timedomain frame obtained afterwards is expanded into two timedomain frames in UOFDMwith similar sizes to the original OFDM frame (Fig 6) Thefirst frame is identical to the original frame while the secondis a flipped replica of the original frame A unipolar OFDMwaveform can be achieved by zero level clipping without theneed of any DC biasing At the receiver each second framewould be subtracted from the first frame of the same pair in order to reconstruct the original bipolar OFDM frame Thiswould double the noise at the receiver which leads to a 3 dBpenalty when compared with bipolar OFDM at equivalent constellation sizes The SE of UOFDM is half of the SE of DCOOFDM since two UOFDM frames are required to convey thesame information conveyed in a single DCOOFDM frame Thesingle tap equalizer can be used for UOFDM providing thatthe ISI effects on the first frame are identical to the ISI effectson the second frame414 Performance of Inherent Unipolar OFDM Techniques

The inherent unipolar OFDM schemes (ACO OFDM U OFDM and FlipOFDM) were introduced as power efficient alternatives to DCOOFDM However because two timedomainUOFDMFlipOFDM frames are required to convey the information contained in a single DCOOFDM frame and because

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 3 Subcarriers mapping of the input frames for DCOOFDMACOOFDM and PAMDMT Xi represents the M QAM symbol atthe i th subcarrier and Pi represents the M PAM symbol at the i thsubcarrier

ACOOFDM asymmetrically clipped optical OFDMDC direct current

DCOOFDM DCbiased optical OFDMPAMDMT pulseamplitudemodulated discrete multitone modulation

Figure 4 The timedomain ACOOFDM waveform

Figure 5 The timedomain PAMDMT waveform

DC X1 X2 X3 0 X 3 X 2 X 1

DCOOFDM Hermitian symmetry

0 X1 0 X3 0 X 3 0 X 1

ACOOFDM Hermitian symmetry

0 P1 P2 P3 0 P3 P2 P1

PAMDMT Hermitian symmetry

0 3 7

2

-2

0 n1051773 ACO(n)

0 1 3

2

-2

0 n

1051773 PAM(n) 1

-1

2Discrete time samples (s)

Discrete time samples (s)

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half of the subcarriers are skipped in ACOOFDM the performance of M QAM DCOOFDM should be compared with theperformance of M2 QAM (ACOOFDM UOFDM and Flip OFDM) Additionally PAMDMT uses M PAM on the imaginary part of the subcarriers instead of MQAM Since the performance of M PAM is equivalent to the performance of M2 QAM the BER of PAMDMT is similar to that of the inherentunipolar schemes When compared with DCO OFDM at thesame SE the performance of all of the inherent unipolarOFDM techniques degrades as the constellation size of M QAM or M PAM increases For example the performance of1024QAM ACOOFDMUOFDMFlipOFDM and 32PAMPAMDMT would be required to be compared with the performance of 32QAM DCOOFDM

Improved receivers for all of the inherent unipolar OFDMtechniques were proposed in [33]-[41] Most of these improvedreceivers would either require a flat channel to operate or incur additional computational complexities Two main methodsare considered in the design of these improved receivers Inthe first method the timedomain symmetry can be exploitedat the receiver to achieve performance gains An amplitudecomparison between the symmetric received signal samplescan improve the receiver detection in flat fading channels atthe expense of increased computational complexity The second method is based on the frequency diversity The even subcarriers in ACOOFDM and the real part of the subcarriers inPAMDMT were exploited respectively to achieve improvedperformance at the receiver [33]-[41] The frequency diversitymethod can be used in the frequency selective channel however it has a higher computational complexity In addition it cannot be used for U OFDMFlip OFDM because both schemesare based on the timedomain processing of the OFDM framesBased on their statistical distribution the inherent unipolar optical OFDM waveforms utilize the lower part of the VL characteristic Therefore these schemes are suitable candidates for LiFi dimmable applications since they can operate with lower optical power dissipation Adaptive bit loading techniques werestudied for MCM techniques DCOOFDM and ACOOFDMand compared with SCFDE in [42] It was found that the per

formance of SC FDE is worse than ACO OFDM but better than DCOOFDM In addition SC FDE is less complex than DCO OFDM and ACOOFDM42 Hybrid OFDM Techniques

OFDM was modified in many studies totailor several specific aspects of the Li Fisystem parameters The natural spatial signal summing in the optical domain was proposed in [43] An array of multiple LEDs isused to transmit the OFDM signal so thatthe subcarriers are allocated to differentLEDs As the number of the LEDs in the ar

ray increases the PAPR of the electrical OFDM signals reduces When the number of subcarriers is equal to the number ofthe LEDs in the array the PAPR would reach its minimum value of 3 dB as the electrical signal would be an ideal sine waveThe spatial optical OFDM (SOOFDM) is reported to haveBER performance gains over DCOOFDM at high SNR due tothe reduced PAPR and the robustness against LED nonlinearities [43] Reverse polarity optical OFDM (RPOOFDM) wasproposed to allow a higher degree of illumination control in theOFDMbased LiFi systems [44] RPOOFDM combines a realvalued optical OFDM broadband technique with slow PWM toallow dimming The dynamic range of the LED is fully used inRPOOFDM to minimize any nonlinear distortion The RPOOFDM is reported to achieve higher performance gains compared with DCOOFDM at a large fraction of dimming rangeswithout limiting the data rate of the system RPOOFDM offersa practical solution for the illumination and dimming controlfor LiFi communication systems however the OFDM signal inRPOOFDM is based on unipolar OFDM This means that theSE of RPOOFDM is half of that of DCOOFDM As a resultthe power efficiency advantage over DCOOFDM starts to diminish as the SE increases In addition the PWM duty cycle isassumed to be known at the receiver which means that sideinformation should be sent before any transmission and this requires perfect synchronization between the transmitting and receiving ends A novel technique that combines ACOOFDM onthe odd subcarriers with DCOOFDM on the even subcarrierswas proposed in asymmetrically DC biased optical OFDM(ADOOFDM) [45] The clipping noise of the ACOOFDM fallsonly into the even subcarriers and can be estimated and canceled with a 3 dB penalty at the receiver The power allocationfor different constellation sizes between ACOOFDM and DCOOFDM streams in ADOOFDM was investigated in [15] Theoptical power efficiency of the optimal settings for ADO OFDM was better than ACOOFDM and DCOOFDM for different configurations Hybrid asymmetrical clipped OFDM (HACOOFDM) uses ACOOFDM on the odd subcarriers and PAMDMT on the even subcarriers to improve the SE of unipolarOFDM modulation techniques [46] The asymmetrical clipping

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 6 (a) Bipolar OFDM waveform (b) UOFDM waveform

0 5 10

5

0

X U[n]

n(b)

0 5

X Bip[n]

5

-5

0 n

(a)Discrete time samples (s) Discrete time samples (s)

+ -

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DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

of the ACOOFDM on the odd symbols would only distort theeven subcarriers At the receiver ACOOFDM symbols are demodulated first by only considering the odd subcarriers andthen remodulated to estimate the ACOOFDM distortion on theeven subcarriers This allows the PAMDMT symbols on theeven subcarrier to be demodulated without any distortion TheSE achieved in HACO OFDM is identical to that of DCO OFDM however PAMDMT uses M PAM modulation on halfof the subcarriers Equal power was allocated to ACOOFDMand PAMDMT As the performance of M2QAM is equivalentto the performance of MPAM the power requirements for bothACOOFDM and PAMDMT to achieve the same performanceis different The problem also appears when different modulation orders are used for both schemes Unequal power allocation for both schemes was investigated in [47] to guarantee thatthe performance of both schemes in HACO OFDM is equalAn improved but computationally complex receiver was alsoproposed in [47] based on the time domain symmetry of bothACOOFDM and PAMDMT

Polar OFDM (POFDM) is a new method to achieve the IMDD for OFDM [48] The main principle of POFDM is to convert the complex valued output of the IFFT from the Cartesiancoordinates into the polar coordinates Therefore the radialand angular coordinate can be sent in the first and secondhalves of the OFDM frame successively It avoids the use ofHermitian symmetry however it allocates the M QAM symbols into the even indexed subcarriers As a result P OFDMhas halfwave even symmetry which states that the first half ofthe complex valued timedomain frame is identical to the otherhalf Therefore it is sufficient to transmit the first half of theIFFT output As a result the SE is reduced to be identical tothat of DCOOFDM since only half of the subcarriers are usedThe performance of P OFDM was compared to that of ACOOFDM in [49] It was reported that P OFDM achieves betterBER performance gains than ACO OFDM under narrow dynamic ranges when optimal values for the power allocation ofthe radial and angular information are used Note that any ISIbetween the radial and angular samples may deteriorate thesystem performance therefore the system performance in frequency selective channels should be investigated Asymmetrical and symmetrical clipping optical OFDM (ASCO OFDM)was proposed in [50] for IMDD Li Fi systems The ACO OFDM is combined with symmetrical clipping optical OFDM(SCOOFDM) that uses the even subcarriers The clipping distortion of both ACOOFDM and SCOOFDM affects the evensubcarriers However the clipping distortion of ACO OFDMcan be estimated and canceled at the receiver The SCO OFDM clipping noise can be removed at the receiver using UOFDMFlip OFDM time domain processing techniques TheSE of ASCOOFDM is 75 of the SE of DCOOFDM ASCOOFDM was reported to have better symbol error rate (SER)compared with ADOOFDM since the ADOOFDM uses theDC bias for the even subcarriers FIR filtering technique

termed spectral factorization was used to create a unipolar optical OFDM signal [51] The amplitude of the subcarriers inspectral factorized optical OFDM (SFOOFDM) were chosen toform an autocorrelation sequence that was shown to be sufficient to guarantee a unipolar OFDM output The SFOOFDMwas reported to achieve 05 dB gain over ACO OFDM with30 PAPR reduction [51] The position modulation OFDM(PMOFDM) avoids the Hermitian symmetry and splits the realand imaginary components of the OFDM output into twobranches where a polarity separator is used to obtain the positive and negative samples of each branch [52] The four framescomposed of a real positive frame a real negative one an imaginary positive one and an imaginary negative one are transmitted as unipolar OFDM frames The SE is exactly similar to other inherent unipolar OFDM techniques discussed in section41 The performance of PMOFDM was reported to be identical to UOFDM in flat channels However it was reported tohave better BER performance when compared to ACOOFDMfor frequency selective channels [52]43 Superposition OFDM Techniques

Superposition OFDM based modulation techniques rely onthe fact that the SE of UOFDMFlipOFDM ACOOFDM andPAMDMT can be doubled by proper superimposing of multiple layers of OFDM waveforms Superposition modulation wasfirst introduced for OFDM based OWC and has led to enhanced UOFDM (eUOFDM) [53] The eUOFDM compensates for the spectral efficiency loss of UOFDM by superimposing multiple UOFDM streams so that the interstreaminterference is null The generation method of the first depth ineUOFDM is exactly similar to that in UOFDM Subsequentdepths can be generated by UOFDM modulators before eachunipolar OFDM frame is repeated 2d1 times and scaled by 12d1where d is the depth number At the receiver the informationconveyed in the first depth is demodulated and then remodulated to be subtracted from the overall received signal Then repeated frames which are equivalent at higher depths are recombined and the demodulation procedure continues the same asfor the stream at the first depth Afterwards the informationconveyed in latter depths is demodulated in a similar way TheSE gap between UOFDM and DCOOFDM can never be completely closed with eU OFDM as this would require a largenumber of information streams to be superimposed in the modulation signal Implementation issues such as latency computational complexity power penalty and memory requirementsput a practical limit on the maximum number of availabledepths The eUOFDM was generalized in the Generalized Enhanced Unipolar OFDM (GREENER OFDM) for configurations where arbitrary constellation sizes and arbitrary power allocations are used [54] As a result the SE gap between U OFDM and DCOOFDM can be closed completely with an appropriate selection of the constellation sizes in different information streams The symmetry in UOFDM lies in frames

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 35

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

7

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

whilst in ACOOFDM and PAMDMT it lies in subframesThe superposition concept has also been extended to other

unipolar OFDM techniques such as PAMDMT [55] and ACOOFDM [56]- [60] The enhanced asymmetrically clipped optical OFDM (eACO OFDM) [56] uses the symmetry of ACO OFDM subframes to allow multiple ACOOFDM streams to besuperimposed A similar concept was also proposed by Elgalaet al and Wang et al under the names of spectrally and energyefficient OFDM (SEEOFDM) [57] and layered asymmetricallyclipped optical OFDM (Layered ACOOFDM) [58] respectively The receiver proposed in SEEOFDM [57] results in SNRpenalty that could have been avoided by using the symmetryproperties of ACOOFDM streams The symmetry arrangementin Layered ACOOFDM [58] is described in the frequency domain however it is shown in [58 Fig2] that it takes place inthe time domain Recently an alternative method to achievesuperposition modulation based on ACOOFDM was proposedby Kozu et al [59] for two ACOOFDM streams and Lawery[60] for Layered ACO OFDM This is similar in principle tothe solutions in [56]- [58] however the superposition is performed in the frequency domain which results in simpler system design The concept of eACO OFDM was generalized toclose the SE gap between ACOOFDM and DCOOFDM Thegeneration of eACOOFDM signal starts at the first depth withan ACOOFDM modulator Additional depths are generated ina similar way to the first depth but with an OFDM framelength equal to half of the previous depth frames Similar to eUOFDM all of the generated frames are repeated 2dminus1 times andappropriately scaled The demodulation process at the receiveris applied in a similar way as the eUOFDM The informationat Depth1 can be recovered directly as in conventional ACOOFDM because all of the inter stream interference falls intothe evenindexed subcarriers After the first stream is decodedthe information can be remodulated again and subtracted fromthe overall received signal Then the frames that are equivalent can be recombined and the demodulation procedure continues as for the stream at first depth

The enhanced pulse amplitude modulated discrete multi tone (ePAMDMT) [55] demonstrates that superposition modulation can also be utilized when the antisymmetry of PAM DMT waveforms is used Analogous to eUOFDM and eACOOFDM unique timedomain structures are also present in PAMDMT If the interference over a single PAMDMT frame possesses a Hermitian symmetry in the timedomain its frequencyprofile falls on the real component of the subcarriers Hencethe interference is completely orthogonal to the useful information which is encoded in imaginary symbols of the PAMDMTframes The concept of superposition modulation was extendedto ePAMDMT for an arbitrary modulation order and an arbitrary power allocation at each depth [55] The theoretical BERanalysis of eACOOFDM is similar to the analysis of GREENEROFDM therefore the optimal modulation sizes and scalingfactors are identical This is an expected result because the

performance of their unipolar OFDM forms ACOOFDM and UOFDM is also similar The ePAMDMT is less energy efficientthan GREENER OFDM and eACO OFDM because ePAMDMT has 3 dB loss in each depth demodulation process andthe optimal configurations of ePAM DMT are suboptimal asthe non squared M QAM BER performance can never beachieved using the M PAM modulation scheme The ePAMDMT is more energy efficient than DCOOFDM in terms of theelectrical SNR at SE values above 1 bitsHz In terms of theoptical SNR the ePAMDMT is less energy efficient than DCOOFDM for all of the presented values Higher optical energydissipation is a desirable property for illumination based LiFiapplications but it is considered as a disadvantage for dimmablebased LiFi applications However GREENEROFDM andeACOOFDM are suitable candidates for dimmablebased LiFi applications due to their optical SNR performance

5 Other MultiCarrier ModulationTechniquesOFDM has been mainly studied in the context of LiFi chan

nels based on FFT Other transformations such as discreteHartley transformation (DHT) [61] wavelet packet divisionmultiplexing (WPDM) [62] and Hadamard coded modulation(HCM) [63] have also been considered for Li Fi channels Amulticarrier IMDD system based on DHT was proposed in[61] It was shown that DHT output can be real when an inputframe of real modulated symbols such as binary phase shiftkeying (BPSK) and M PAM is used Similar to DCOOFDMand ACOOFDM DCbiasing and asymmetrical clipping canalso be used to achieve unipolar output in DHTbased multicarrier modulation technique As a major advantage over FFTbased conventional OFDM the DHTbased multicarrier modulation does not require any Hermitian symmetry However thisfails to improve the SE as real modulated symbols such as MPAM are used in DHTbased multicarrier modulation WPDMuses orthogonal wavelet packet functions for symbol modulation where the basis functions are wavelet packet functionswith finite length It was reported that the performance of WPDM is better than that of OFDM in terms of the spectral andpower efficiencies when LED nonlinear distortion and channeldispersion are taken into account [62] The high illuminationlevel of OFDM Li Fi systems require higher optical powerwhich may result in clipping due to the peak power constraintof the VL transfer function of the LED (Fig 2) HCM was proposed for multicarrier modulation LiFi as a solution to the limitation of OFDM modulation at higher illumination levels Thetechnique is based on fast Walsh Hadamard transformation(FWHT) as an alternative to the FFT HCM is reported toachieve higher performance gains when compared with ACOOFDM and DCO OFDM at higher illumination levels [63]However the performance improvement over RPO OFDM ismodest An alternative variant of HCM termed DC reduced

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS36

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

8

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 2: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

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Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS30

strictly positive signals Single carrier modulation (SCM) techniques are straight forward to implement in LiFi Modulationtechniques such as onoff keying (OOK) pulseposition modulation (PPM) and M ary pulse amplitude modulation (M PAM) can be easily implemented However due to the dispersive nature of optical wireless channels such schemes requirecomplex equalizers at the receiver Therefore the performanceof these schemes degrades as their spectral efficiency (SE) increases On the other hand multiple carrier modulation (MCM)techniques such as the orthogonal frequency division multiplexing (OFDM) have been shown to be potential candidatesfor optical wireless channels since they only require single tapequalizer at the receiver Adaptive bit and power loading canmaximize the achievable data rates of OFDMbased LiFi systems by adapting the system loading to the channel frequencyresponse Moreover the DC wander and low frequency interference can be easily avoided in OFDM by optimizing the adaptive bitpower loading to avoid the low frequency subcarriersColour modulation techniques are unique to LiFi communication systems as the information is modulated on the instantaneous colour changes The colour dimension adds a new degree of freedom to LiFi The various modulation LiFi modulation techniques discussed in this paper are shown in Fig 1

This paper is organized as follows The main challenges forLi Fi modulation techniques are summarized in Section 2SCM techniques for Li Fi are detailed in Section 3 OFDMbased modulation techniques for LiFi are discussed in detailsin Section 4 including inherent unipolar OFDM techniqueshybrid OFDM modulation techniques and superpositionOFDM modulation techniques Other MCM techniques are revised in Section 5 The unique colour domain modulation techniques are discussed in Section 6 Finally the conclusion ispresented in Section 7 The paper is limited to single input single output (SISO) LiFi communication systems The spacedimension of LiFi is not considered in this paper

2 LiFi Modulation Techniques ChallengesLi Fi is an emerging high speed low cost solution to the

scarcity of the radio frequency (RF) spectrum therefore it is expected to be realized using the widely deployed off the shelfoptoelectronic LEDs Due to the mass production of these inexpensive devices they lack accurate characterizations In LiFilight is modulated on the subtle changes of the light intensitytherefore the communication link would be affected by the nonlinearity of the voltageluminance characteristic As a solution

ACOOFDM asymmetrically clipped optical OFDMADOOFDM asymmetrically clipped DC biased optical OFDM

ASCOOFDM asymmetrically and symmetricallyclipped optical OFDM

CAP carrierless amplitude modulationCIM colour intensity modulationCSK colour shift keying

DCOOFDM DC biased OFDMDFTsOFDM discrete Fourier transformation spread OFDM

DHT discrete Hartley transformeACOOFDM enhanced ACOOFDM

ePAMDMT enhanced PAMDMTeUOFDM enhanced unipolar OFDM

HACOOFDM hybrid asymmetrically clippedoptical OFDM

HCM Hadamard coded modulationLACOOFDM layered ACOOFDM

LiFi light fidelityMCM multicarrier modulationMM metameric modulation

MPAM Mary pulse amplitude modulationMPPM Mary pulse position modulation

OFDM orthogonal frequency modulationOOK onoff keying

PAMDMT pulse amplitude modulation discrete multitonePMOFDM position modulation OFDMPOFDM polar OFDM

PWM pulse width modulationRPOOFDM reverse polarity optical OFDM

SCM single carrier modulationSEEOFDM spectrally and energy efficient OFDMSFOOFDM spectrally factorized optical OFDM

WPDM wavelet packet division multiplexingFigure 1 LiFi modulation techniques considered in this paper

LiFi modulation tech

SCM

OOK

PWM

MPAM

MPPM

DFTsOFDM

CAP

DCOOFDM InherentunipolarACOOFDM

PAMDMT

UOFDM

SuperpositionOFDMeUOFDM

eACOOFDM

ePAMDMT

SEEOFDM

LACOOFDM

Hybrid

RPOOFDM

POFDM

SpatialOFDM

ASCOOFDM

SFOOFDM

PMOFDM

ADOOFDM

HACOOFDM

Other MCM

HCM

WPDM

DHT

Colour domainMod

CSK

CIM

MM

OFDM (MCM)

2

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

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April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 31

predistortion techniques were proposed to mitigate nonlineardistortion [4] However as the LED temperature increases thevoltageluminance (VL) characteristic experiences memoryeffects Therefore the LED non linearity mitigation is still anopen research problem The limited bandwidth of LiFi communication channel leads to inter symbol interference (ISI) athigh data rates The LED frequency response is modeled as alowpass filter and it is the major contributor to the frequencyselectivity of Li Fi channels The modulation bandwidth overwhich the frequency response of most commercially availableLEDs can be considered flat is around 2-20 MHz [5] [6] However the usable bandwidth in LiFi could be extended beyondthe 3 dB cutoff frequency

Therefore modulation techniques with higher spectral efficiencies are key elements in a LiFi system design Satisfyingthe illumination requirements is a key element in LiFi Mostof the research on modulation techniques has been on the communication system performance of Li Fi system Factors suchas dimming illumination level control and flickering havebeen analyzed as secondary parameters of a LiFi system TheLiFi systems should be also considered as an illumination system with communications capability not the reverse

3 Single Carrier Modulation TechniquesSingle carrier modulation techniques were first proposed for

IMDD optical wireless communications based on infrared communications [7] Modulation techniques such as OOK pulseamplitude modulation (PAM) pulse width modulation (PWM)and PPM are straightforward to implement for Li Fi systemsIn general single carrier modulation techniques are suitablecandidates for LiFi when lowtomoderate data rates applications are required By switching the LED betweenldquoonrdquoandldquooffrdquostates the incoming bits can be modulated into the lightintensity Illumination control can be supported by adjustingthe light intensities of theldquoonrdquoandldquooffrdquostates without affecting the system performance Compensation symbols are proposed in the visible light communications standard IEEE802157 [8] to facilitate the illumination control at the expense of reducing the SE If the link budget offers high signalto noise ratios (SNR) MPAM can be used to modulate the incoming bits on the amplitude of the optical pulse [9]The position of the optical pulse is modulated into shorter durationchips in PPM with a position index that varies depending onthe incoming bits The PPM is more power efficient than OOKhowever it requires more bandwidth than OOK to supportequivalent data rates Differential PPM (DPPM) was proposedto achieve power andor SE gains [10] however the effect of unequal bit duration for the different incoming symbols could affect the illumination performance A solution was proposed in[11] to ensure that the duty cycle is similar among the differentsymbols to prevent any possible flickering Variable PPM(VPPM) was proposed in the VLC standard IEEE 802157 to

support dimming for the PPM technique and prevent any possible flickering The pulse dimming in VPPM is controlled bythe width of the pulse rather than the pulse amplitude Therefore VPPM can be considered as a combination of PPM andPWM techniques Multiple PPM (MPPM) was proposed [12] asa solution to the dimming capability of PPM where it was reported that it achieves higher spectral efficiencies than VPPMwith less optical power dissipation The advantages of PAMand PPM are combined in pulse amplitude and position modulation (PAPM) [13]

The performance comparison between single carrier andmulticarrier modulation techniques was studied in [14]- [18]for different scenarios and considerations The results may differ depending on the major considerations and assumptions ofeach study However in general the performance of single carrier modulation techniques deteriorate as the data rates increase due to the increased ISI Equalization techniques suchas optimum maximum likelihood sequence detection (MLSD)frequency domain equalizers (FDE) nonlinear decision feedback equalizers (DFE) and linear feed forward equalizer(FFE) are suitable candidates for equalization processes withdifferent degrees of performance and computational complexity[7] [19] [20] The single carrier frequency domain equalizer(SCFDE) was proposed for OWC as a solution to the high peakto average power ratio (PAPR) of OFDM in [12] [21] PPM SCFDE was considered in [22] and OOKSCFDE was considered in [23] The performance of OOK with minimum meansquare error equalization (MMSE) was compared with the performance of asymmetrically clipped optical (ACO)OFDM andthe performance of complex modulation Mary quadrature amplitude modulation (MQAM) ACOSCFDE in [18] It was reported that the performance of ACOSCFDE outperforms asymmetrically clipped optical OFDM (ACO OFDM) and OOK MMSE due to the high PAPR of ACOOFDM when the nonlinear characteristics of the LED are considered The performance of PAMSCFDE is compared with OFDM in [12] without consideration of the LED nonlinearity It was shown thatPAM SCFDE achieves higher performance gains when compared with OFDM at spectral efficiencies less than 3 bitssHz

Discrete Fourier transformation spread (DFTs) OFDM wasalso considered for LiFi as a SCM that has the benefits of anOFDM multicarrier system with lower PAPR [24] An extrapair of DFT and inverse discrete Fourier transformation (IDFT)operations are required to achieve DFTs OFDM Multiple independent streams of DFTs OFDM modulated waveforms areseparately transmitted through multiple LEDs in a single arrayThe performance of DFTs OFDM is reported to be better whencompared with DC biased optical OFDM (DCO OFDM) interms of both PAPR and bit error rate (BER) [24] A novel carrierless amplitude and phase (CAP) modulation was proposedfor Li Fi in [25] In order for CAP to suit the frequency response of LEDs the spectrum of CAP was divided into m subcarriers by the aid of finite impulse response (FIR) filter Al

3

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

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April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS32

though CAP is computationally complex it could offer highspectral efficiencies in bandlimited LiFi channel

4 Optical OFDMSingle carrier modulation techniques require a complex

equalization process when employed at high data rates In addition effects such as DC wandering and flickering interferenceof florescent lights may influence the system performance atthe lower frequency regions of the used bandwidth On the other hand multicarrier modulation techniques such as OFDMcan convert the frequency selective fading of the communication channel into a flat fading by employing the computationally efficient single tap equalizer In addition OFDM supportsadaptive power and bit loading which can adapt the channelutilization to the frequency response of the channel This canmaximize the system performance Supporting multiuser communication systems is an inherent advantage of OFDM whereeach user could be allocated certain subcarriers At the OFDMtransmitter the incoming bits are modulated into specific modulation formats such as M QAM The M QAM symbols areloaded afterwards into orthogonal subcarriers with subcarrierspacing equal to multiple of the symbol duration The parallelsymbols can then be multiplexed into a serial time domain output generally using inverse fast Fourier transformation (IFFT)The physical link of LiFi is achieved using offtheshelf optoelectronic devices such as LED and photodetectors (PD) Dueto the fact that these light sources produce an incoherent lightthe OFDM timedomain waveforms are used in LiFi to modulate the intensity of the LED source Therefore these waveforms are required to be both unipolar and real valued

Hermitian symmetry is generally imposed on the OFDM input frame to enforce the OFDM time domain signal output intothe real domain Different variants of optical OFDM were proposed to achieve a unipolar OFDM output DC bias is used inthe widely deployed DCOOFDM [26] to realize a unipolar timedomain OFDM output However OFDM signals have a highPAPR which makes it practically impossible to convert all ofthe signal samples into unipolar ones The OFDM timedomainwaveform can be approximated with a Normal distributionwhen the length of the input frame is greater than 64 The DCbias point would be dependent on the VL characteristic of theLED Zero level clipping of the remaining negative samples after the biasing would result in a clipping distortion that coulddeteriorate the system performance High DC bias would alsoincur some distortion as a result of the upper clipping of theOFDM waveform due to the V L characteristic of the idealLED The forward output current characteristic of an LED isshown in Fig 2 Predistortion is used to linearize the dynamicrange of the LED The LED input and output probability distribution function (PDF) of the OFDM modulation signal are alsoshown The dynamic range of the LED is between the turnonbias and the maximum allowed current points of the LED The

input signal is biased and the output signal is clipped for values outside the dynamic range The optimization of the DC biasing point was studied in [27]- [29] The additional dissipation of electrical power in DCOOFDM compared with bipolarOFDM increases as the modulation order increases This leadsto electrical and optical power inefficiency when DCOOFDMis used with high M QAM modulation orders Illumination isan essential part of VLC therefore the DCO OFDM opticalpower inefficiency can be justified for some VLC applicationsHowever when energy efficiency is required an alternativemodulation approach is required41 Inherent Unipolar Optical OFDM Techniques

Unipolar OFDM modulation schemes were mainly introduced to provide energy efficient optical OFDM alternatives toDCOOFDM These schemes include ACOOFDM [30] pulseamplitude modulated discrete multitone modulation (PAM DMT) [31] flipped OFDM (FlipOFDM) [32] and unipolar orthogonal frequency division multiplexing (UOFDM) [33] Theyexploit the OFDM inputoutput frame structure to produce aunipolar time domain waveform output However all of theseschemes have a reduced SE compared with DCOOFDM due tothe restrictions imposed on their frame structures In this section ACOOFDM PAMDMT and UOFDMFlipOFDM modulation schemes are discussed411 ACOOFDM

A real unipolar OFDM waveform can be achieved by exploiting the Fourier transformation properties on the frequency domain input OFDM frames The principle of ACOOFDM [30] isto skip the even subcarriers of an OFDM frame by only loading the odd subcarriers with useful information (Fig 3) Thiscreates a symmetry in the time domain OFDM signal which al

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

LED light emitting diode PDF probability distribution functionFigure 2 The forwardoutput current characteristic of an LED

I f

I out

LED transfer function

After predistortion

Dynamic rangeInput PDF

Output PDF

4

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 33

lows the distortionless clipping of the negative samples without the need of any DC biasing (Fig 4) Clipping of the negative values is distortionless since all of the distortion will onlyaffect the evenindexed subcarriers However skipping half ofthe subcarriers reduces the SE of ACOOFDM to half of that inDCOOFDM A penalty of 3 dB should applied to the signaltonoise ratio (SNR) of ACOOFDM when compared with bipolarOFDM since half of the signal power is lost due to clippingHermitian symmetry is also used to guarantee a real valuedACOOFDM output At the receiver after a fast Fourier transformation (FFT) is applied on the incoming frame only oddsubcarriers are considered412 PAMDMT

A real unipolar optical OFDM is realized in PAMDMT byexploiting the Fourier properties of imaginary signals The realcomponent of the subcarriers is not used in PAMDMT whichrestricts the modulation scheme used to MPAM (Fig 3) Byonly loading MPAM modulated symbols on the imaginary components of the subcarriers an antisymmetry in the time domain waveform of PAMDMT would be achieved (Fig 5) Thiswould facilitate the distortionless zero level clipping of PAMDMT waveform as all of the distortion would only affect the re

al component of the subcarriers Hermitian symmetry is alsoused to guarantee a real valued PAMDMT output PAMDMTis more attractive than ACO OFDM when bit loading techniques are considered as the PAMDMT performance can beoptimally adapted to the frequency response of the channelsince all of the subcarriers are used The SE of PAMDMT issimilar to that of DCOOFDM PAMDMT has a 3 dB fixedpenalty when compared with bipolar OFDM at an appropriateconstellation size as half of the power is also lost due to clipping At the receiver the imaginary part of the subcarriers isonly considered while the real part is ignored413 UOFDMFlipOFDM

The concept and performance of UOFDM and FlipOFDMis identical In this paper the term UOFDM is used howeverall discussion and analysis is applicable to both schemes Hermitian symmetry is applied on the incoming frame of MQAMsymbols The bipolar OFDM timedomain frame obtained afterwards is expanded into two timedomain frames in UOFDMwith similar sizes to the original OFDM frame (Fig 6) Thefirst frame is identical to the original frame while the secondis a flipped replica of the original frame A unipolar OFDMwaveform can be achieved by zero level clipping without theneed of any DC biasing At the receiver each second framewould be subtracted from the first frame of the same pair in order to reconstruct the original bipolar OFDM frame Thiswould double the noise at the receiver which leads to a 3 dBpenalty when compared with bipolar OFDM at equivalent constellation sizes The SE of UOFDM is half of the SE of DCOOFDM since two UOFDM frames are required to convey thesame information conveyed in a single DCOOFDM frame Thesingle tap equalizer can be used for UOFDM providing thatthe ISI effects on the first frame are identical to the ISI effectson the second frame414 Performance of Inherent Unipolar OFDM Techniques

The inherent unipolar OFDM schemes (ACO OFDM U OFDM and FlipOFDM) were introduced as power efficient alternatives to DCOOFDM However because two timedomainUOFDMFlipOFDM frames are required to convey the information contained in a single DCOOFDM frame and because

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 3 Subcarriers mapping of the input frames for DCOOFDMACOOFDM and PAMDMT Xi represents the M QAM symbol atthe i th subcarrier and Pi represents the M PAM symbol at the i thsubcarrier

ACOOFDM asymmetrically clipped optical OFDMDC direct current

DCOOFDM DCbiased optical OFDMPAMDMT pulseamplitudemodulated discrete multitone modulation

Figure 4 The timedomain ACOOFDM waveform

Figure 5 The timedomain PAMDMT waveform

DC X1 X2 X3 0 X 3 X 2 X 1

DCOOFDM Hermitian symmetry

0 X1 0 X3 0 X 3 0 X 1

ACOOFDM Hermitian symmetry

0 P1 P2 P3 0 P3 P2 P1

PAMDMT Hermitian symmetry

0 3 7

2

-2

0 n1051773 ACO(n)

0 1 3

2

-2

0 n

1051773 PAM(n) 1

-1

2Discrete time samples (s)

Discrete time samples (s)

5

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

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April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS34

half of the subcarriers are skipped in ACOOFDM the performance of M QAM DCOOFDM should be compared with theperformance of M2 QAM (ACOOFDM UOFDM and Flip OFDM) Additionally PAMDMT uses M PAM on the imaginary part of the subcarriers instead of MQAM Since the performance of M PAM is equivalent to the performance of M2 QAM the BER of PAMDMT is similar to that of the inherentunipolar schemes When compared with DCO OFDM at thesame SE the performance of all of the inherent unipolarOFDM techniques degrades as the constellation size of M QAM or M PAM increases For example the performance of1024QAM ACOOFDMUOFDMFlipOFDM and 32PAMPAMDMT would be required to be compared with the performance of 32QAM DCOOFDM

Improved receivers for all of the inherent unipolar OFDMtechniques were proposed in [33]-[41] Most of these improvedreceivers would either require a flat channel to operate or incur additional computational complexities Two main methodsare considered in the design of these improved receivers Inthe first method the timedomain symmetry can be exploitedat the receiver to achieve performance gains An amplitudecomparison between the symmetric received signal samplescan improve the receiver detection in flat fading channels atthe expense of increased computational complexity The second method is based on the frequency diversity The even subcarriers in ACOOFDM and the real part of the subcarriers inPAMDMT were exploited respectively to achieve improvedperformance at the receiver [33]-[41] The frequency diversitymethod can be used in the frequency selective channel however it has a higher computational complexity In addition it cannot be used for U OFDMFlip OFDM because both schemesare based on the timedomain processing of the OFDM framesBased on their statistical distribution the inherent unipolar optical OFDM waveforms utilize the lower part of the VL characteristic Therefore these schemes are suitable candidates for LiFi dimmable applications since they can operate with lower optical power dissipation Adaptive bit loading techniques werestudied for MCM techniques DCOOFDM and ACOOFDMand compared with SCFDE in [42] It was found that the per

formance of SC FDE is worse than ACO OFDM but better than DCOOFDM In addition SC FDE is less complex than DCO OFDM and ACOOFDM42 Hybrid OFDM Techniques

OFDM was modified in many studies totailor several specific aspects of the Li Fisystem parameters The natural spatial signal summing in the optical domain was proposed in [43] An array of multiple LEDs isused to transmit the OFDM signal so thatthe subcarriers are allocated to differentLEDs As the number of the LEDs in the ar

ray increases the PAPR of the electrical OFDM signals reduces When the number of subcarriers is equal to the number ofthe LEDs in the array the PAPR would reach its minimum value of 3 dB as the electrical signal would be an ideal sine waveThe spatial optical OFDM (SOOFDM) is reported to haveBER performance gains over DCOOFDM at high SNR due tothe reduced PAPR and the robustness against LED nonlinearities [43] Reverse polarity optical OFDM (RPOOFDM) wasproposed to allow a higher degree of illumination control in theOFDMbased LiFi systems [44] RPOOFDM combines a realvalued optical OFDM broadband technique with slow PWM toallow dimming The dynamic range of the LED is fully used inRPOOFDM to minimize any nonlinear distortion The RPOOFDM is reported to achieve higher performance gains compared with DCOOFDM at a large fraction of dimming rangeswithout limiting the data rate of the system RPOOFDM offersa practical solution for the illumination and dimming controlfor LiFi communication systems however the OFDM signal inRPOOFDM is based on unipolar OFDM This means that theSE of RPOOFDM is half of that of DCOOFDM As a resultthe power efficiency advantage over DCOOFDM starts to diminish as the SE increases In addition the PWM duty cycle isassumed to be known at the receiver which means that sideinformation should be sent before any transmission and this requires perfect synchronization between the transmitting and receiving ends A novel technique that combines ACOOFDM onthe odd subcarriers with DCOOFDM on the even subcarrierswas proposed in asymmetrically DC biased optical OFDM(ADOOFDM) [45] The clipping noise of the ACOOFDM fallsonly into the even subcarriers and can be estimated and canceled with a 3 dB penalty at the receiver The power allocationfor different constellation sizes between ACOOFDM and DCOOFDM streams in ADOOFDM was investigated in [15] Theoptical power efficiency of the optimal settings for ADO OFDM was better than ACOOFDM and DCOOFDM for different configurations Hybrid asymmetrical clipped OFDM (HACOOFDM) uses ACOOFDM on the odd subcarriers and PAMDMT on the even subcarriers to improve the SE of unipolarOFDM modulation techniques [46] The asymmetrical clipping

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 6 (a) Bipolar OFDM waveform (b) UOFDM waveform

0 5 10

5

0

X U[n]

n(b)

0 5

X Bip[n]

5

-5

0 n

(a)Discrete time samples (s) Discrete time samples (s)

+ -

6

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

of the ACOOFDM on the odd symbols would only distort theeven subcarriers At the receiver ACOOFDM symbols are demodulated first by only considering the odd subcarriers andthen remodulated to estimate the ACOOFDM distortion on theeven subcarriers This allows the PAMDMT symbols on theeven subcarrier to be demodulated without any distortion TheSE achieved in HACO OFDM is identical to that of DCO OFDM however PAMDMT uses M PAM modulation on halfof the subcarriers Equal power was allocated to ACOOFDMand PAMDMT As the performance of M2QAM is equivalentto the performance of MPAM the power requirements for bothACOOFDM and PAMDMT to achieve the same performanceis different The problem also appears when different modulation orders are used for both schemes Unequal power allocation for both schemes was investigated in [47] to guarantee thatthe performance of both schemes in HACO OFDM is equalAn improved but computationally complex receiver was alsoproposed in [47] based on the time domain symmetry of bothACOOFDM and PAMDMT

Polar OFDM (POFDM) is a new method to achieve the IMDD for OFDM [48] The main principle of POFDM is to convert the complex valued output of the IFFT from the Cartesiancoordinates into the polar coordinates Therefore the radialand angular coordinate can be sent in the first and secondhalves of the OFDM frame successively It avoids the use ofHermitian symmetry however it allocates the M QAM symbols into the even indexed subcarriers As a result P OFDMhas halfwave even symmetry which states that the first half ofthe complex valued timedomain frame is identical to the otherhalf Therefore it is sufficient to transmit the first half of theIFFT output As a result the SE is reduced to be identical tothat of DCOOFDM since only half of the subcarriers are usedThe performance of P OFDM was compared to that of ACOOFDM in [49] It was reported that P OFDM achieves betterBER performance gains than ACO OFDM under narrow dynamic ranges when optimal values for the power allocation ofthe radial and angular information are used Note that any ISIbetween the radial and angular samples may deteriorate thesystem performance therefore the system performance in frequency selective channels should be investigated Asymmetrical and symmetrical clipping optical OFDM (ASCO OFDM)was proposed in [50] for IMDD Li Fi systems The ACO OFDM is combined with symmetrical clipping optical OFDM(SCOOFDM) that uses the even subcarriers The clipping distortion of both ACOOFDM and SCOOFDM affects the evensubcarriers However the clipping distortion of ACO OFDMcan be estimated and canceled at the receiver The SCO OFDM clipping noise can be removed at the receiver using UOFDMFlip OFDM time domain processing techniques TheSE of ASCOOFDM is 75 of the SE of DCOOFDM ASCOOFDM was reported to have better symbol error rate (SER)compared with ADOOFDM since the ADOOFDM uses theDC bias for the even subcarriers FIR filtering technique

termed spectral factorization was used to create a unipolar optical OFDM signal [51] The amplitude of the subcarriers inspectral factorized optical OFDM (SFOOFDM) were chosen toform an autocorrelation sequence that was shown to be sufficient to guarantee a unipolar OFDM output The SFOOFDMwas reported to achieve 05 dB gain over ACO OFDM with30 PAPR reduction [51] The position modulation OFDM(PMOFDM) avoids the Hermitian symmetry and splits the realand imaginary components of the OFDM output into twobranches where a polarity separator is used to obtain the positive and negative samples of each branch [52] The four framescomposed of a real positive frame a real negative one an imaginary positive one and an imaginary negative one are transmitted as unipolar OFDM frames The SE is exactly similar to other inherent unipolar OFDM techniques discussed in section41 The performance of PMOFDM was reported to be identical to UOFDM in flat channels However it was reported tohave better BER performance when compared to ACOOFDMfor frequency selective channels [52]43 Superposition OFDM Techniques

Superposition OFDM based modulation techniques rely onthe fact that the SE of UOFDMFlipOFDM ACOOFDM andPAMDMT can be doubled by proper superimposing of multiple layers of OFDM waveforms Superposition modulation wasfirst introduced for OFDM based OWC and has led to enhanced UOFDM (eUOFDM) [53] The eUOFDM compensates for the spectral efficiency loss of UOFDM by superimposing multiple UOFDM streams so that the interstreaminterference is null The generation method of the first depth ineUOFDM is exactly similar to that in UOFDM Subsequentdepths can be generated by UOFDM modulators before eachunipolar OFDM frame is repeated 2d1 times and scaled by 12d1where d is the depth number At the receiver the informationconveyed in the first depth is demodulated and then remodulated to be subtracted from the overall received signal Then repeated frames which are equivalent at higher depths are recombined and the demodulation procedure continues the same asfor the stream at the first depth Afterwards the informationconveyed in latter depths is demodulated in a similar way TheSE gap between UOFDM and DCOOFDM can never be completely closed with eU OFDM as this would require a largenumber of information streams to be superimposed in the modulation signal Implementation issues such as latency computational complexity power penalty and memory requirementsput a practical limit on the maximum number of availabledepths The eUOFDM was generalized in the Generalized Enhanced Unipolar OFDM (GREENER OFDM) for configurations where arbitrary constellation sizes and arbitrary power allocations are used [54] As a result the SE gap between U OFDM and DCOOFDM can be closed completely with an appropriate selection of the constellation sizes in different information streams The symmetry in UOFDM lies in frames

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 35

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

7

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

whilst in ACOOFDM and PAMDMT it lies in subframesThe superposition concept has also been extended to other

unipolar OFDM techniques such as PAMDMT [55] and ACOOFDM [56]- [60] The enhanced asymmetrically clipped optical OFDM (eACO OFDM) [56] uses the symmetry of ACO OFDM subframes to allow multiple ACOOFDM streams to besuperimposed A similar concept was also proposed by Elgalaet al and Wang et al under the names of spectrally and energyefficient OFDM (SEEOFDM) [57] and layered asymmetricallyclipped optical OFDM (Layered ACOOFDM) [58] respectively The receiver proposed in SEEOFDM [57] results in SNRpenalty that could have been avoided by using the symmetryproperties of ACOOFDM streams The symmetry arrangementin Layered ACOOFDM [58] is described in the frequency domain however it is shown in [58 Fig2] that it takes place inthe time domain Recently an alternative method to achievesuperposition modulation based on ACOOFDM was proposedby Kozu et al [59] for two ACOOFDM streams and Lawery[60] for Layered ACO OFDM This is similar in principle tothe solutions in [56]- [58] however the superposition is performed in the frequency domain which results in simpler system design The concept of eACO OFDM was generalized toclose the SE gap between ACOOFDM and DCOOFDM Thegeneration of eACOOFDM signal starts at the first depth withan ACOOFDM modulator Additional depths are generated ina similar way to the first depth but with an OFDM framelength equal to half of the previous depth frames Similar to eUOFDM all of the generated frames are repeated 2dminus1 times andappropriately scaled The demodulation process at the receiveris applied in a similar way as the eUOFDM The informationat Depth1 can be recovered directly as in conventional ACOOFDM because all of the inter stream interference falls intothe evenindexed subcarriers After the first stream is decodedthe information can be remodulated again and subtracted fromthe overall received signal Then the frames that are equivalent can be recombined and the demodulation procedure continues as for the stream at first depth

The enhanced pulse amplitude modulated discrete multi tone (ePAMDMT) [55] demonstrates that superposition modulation can also be utilized when the antisymmetry of PAM DMT waveforms is used Analogous to eUOFDM and eACOOFDM unique timedomain structures are also present in PAMDMT If the interference over a single PAMDMT frame possesses a Hermitian symmetry in the timedomain its frequencyprofile falls on the real component of the subcarriers Hencethe interference is completely orthogonal to the useful information which is encoded in imaginary symbols of the PAMDMTframes The concept of superposition modulation was extendedto ePAMDMT for an arbitrary modulation order and an arbitrary power allocation at each depth [55] The theoretical BERanalysis of eACOOFDM is similar to the analysis of GREENEROFDM therefore the optimal modulation sizes and scalingfactors are identical This is an expected result because the

performance of their unipolar OFDM forms ACOOFDM and UOFDM is also similar The ePAMDMT is less energy efficientthan GREENER OFDM and eACO OFDM because ePAMDMT has 3 dB loss in each depth demodulation process andthe optimal configurations of ePAM DMT are suboptimal asthe non squared M QAM BER performance can never beachieved using the M PAM modulation scheme The ePAMDMT is more energy efficient than DCOOFDM in terms of theelectrical SNR at SE values above 1 bitsHz In terms of theoptical SNR the ePAMDMT is less energy efficient than DCOOFDM for all of the presented values Higher optical energydissipation is a desirable property for illumination based LiFiapplications but it is considered as a disadvantage for dimmablebased LiFi applications However GREENEROFDM andeACOOFDM are suitable candidates for dimmablebased LiFi applications due to their optical SNR performance

5 Other MultiCarrier ModulationTechniquesOFDM has been mainly studied in the context of LiFi chan

nels based on FFT Other transformations such as discreteHartley transformation (DHT) [61] wavelet packet divisionmultiplexing (WPDM) [62] and Hadamard coded modulation(HCM) [63] have also been considered for Li Fi channels Amulticarrier IMDD system based on DHT was proposed in[61] It was shown that DHT output can be real when an inputframe of real modulated symbols such as binary phase shiftkeying (BPSK) and M PAM is used Similar to DCOOFDMand ACOOFDM DCbiasing and asymmetrical clipping canalso be used to achieve unipolar output in DHTbased multicarrier modulation technique As a major advantage over FFTbased conventional OFDM the DHTbased multicarrier modulation does not require any Hermitian symmetry However thisfails to improve the SE as real modulated symbols such as MPAM are used in DHTbased multicarrier modulation WPDMuses orthogonal wavelet packet functions for symbol modulation where the basis functions are wavelet packet functionswith finite length It was reported that the performance of WPDM is better than that of OFDM in terms of the spectral andpower efficiencies when LED nonlinear distortion and channeldispersion are taken into account [62] The high illuminationlevel of OFDM Li Fi systems require higher optical powerwhich may result in clipping due to the peak power constraintof the VL transfer function of the LED (Fig 2) HCM was proposed for multicarrier modulation LiFi as a solution to the limitation of OFDM modulation at higher illumination levels Thetechnique is based on fast Walsh Hadamard transformation(FWHT) as an alternative to the FFT HCM is reported toachieve higher performance gains when compared with ACOOFDM and DCO OFDM at higher illumination levels [63]However the performance improvement over RPO OFDM ismodest An alternative variant of HCM termed DC reduced

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS36

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

8

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 3: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 31

predistortion techniques were proposed to mitigate nonlineardistortion [4] However as the LED temperature increases thevoltageluminance (VL) characteristic experiences memoryeffects Therefore the LED non linearity mitigation is still anopen research problem The limited bandwidth of LiFi communication channel leads to inter symbol interference (ISI) athigh data rates The LED frequency response is modeled as alowpass filter and it is the major contributor to the frequencyselectivity of Li Fi channels The modulation bandwidth overwhich the frequency response of most commercially availableLEDs can be considered flat is around 2-20 MHz [5] [6] However the usable bandwidth in LiFi could be extended beyondthe 3 dB cutoff frequency

Therefore modulation techniques with higher spectral efficiencies are key elements in a LiFi system design Satisfyingthe illumination requirements is a key element in LiFi Mostof the research on modulation techniques has been on the communication system performance of Li Fi system Factors suchas dimming illumination level control and flickering havebeen analyzed as secondary parameters of a LiFi system TheLiFi systems should be also considered as an illumination system with communications capability not the reverse

3 Single Carrier Modulation TechniquesSingle carrier modulation techniques were first proposed for

IMDD optical wireless communications based on infrared communications [7] Modulation techniques such as OOK pulseamplitude modulation (PAM) pulse width modulation (PWM)and PPM are straightforward to implement for Li Fi systemsIn general single carrier modulation techniques are suitablecandidates for LiFi when lowtomoderate data rates applications are required By switching the LED betweenldquoonrdquoandldquooffrdquostates the incoming bits can be modulated into the lightintensity Illumination control can be supported by adjustingthe light intensities of theldquoonrdquoandldquooffrdquostates without affecting the system performance Compensation symbols are proposed in the visible light communications standard IEEE802157 [8] to facilitate the illumination control at the expense of reducing the SE If the link budget offers high signalto noise ratios (SNR) MPAM can be used to modulate the incoming bits on the amplitude of the optical pulse [9]The position of the optical pulse is modulated into shorter durationchips in PPM with a position index that varies depending onthe incoming bits The PPM is more power efficient than OOKhowever it requires more bandwidth than OOK to supportequivalent data rates Differential PPM (DPPM) was proposedto achieve power andor SE gains [10] however the effect of unequal bit duration for the different incoming symbols could affect the illumination performance A solution was proposed in[11] to ensure that the duty cycle is similar among the differentsymbols to prevent any possible flickering Variable PPM(VPPM) was proposed in the VLC standard IEEE 802157 to

support dimming for the PPM technique and prevent any possible flickering The pulse dimming in VPPM is controlled bythe width of the pulse rather than the pulse amplitude Therefore VPPM can be considered as a combination of PPM andPWM techniques Multiple PPM (MPPM) was proposed [12] asa solution to the dimming capability of PPM where it was reported that it achieves higher spectral efficiencies than VPPMwith less optical power dissipation The advantages of PAMand PPM are combined in pulse amplitude and position modulation (PAPM) [13]

The performance comparison between single carrier andmulticarrier modulation techniques was studied in [14]- [18]for different scenarios and considerations The results may differ depending on the major considerations and assumptions ofeach study However in general the performance of single carrier modulation techniques deteriorate as the data rates increase due to the increased ISI Equalization techniques suchas optimum maximum likelihood sequence detection (MLSD)frequency domain equalizers (FDE) nonlinear decision feedback equalizers (DFE) and linear feed forward equalizer(FFE) are suitable candidates for equalization processes withdifferent degrees of performance and computational complexity[7] [19] [20] The single carrier frequency domain equalizer(SCFDE) was proposed for OWC as a solution to the high peakto average power ratio (PAPR) of OFDM in [12] [21] PPM SCFDE was considered in [22] and OOKSCFDE was considered in [23] The performance of OOK with minimum meansquare error equalization (MMSE) was compared with the performance of asymmetrically clipped optical (ACO)OFDM andthe performance of complex modulation Mary quadrature amplitude modulation (MQAM) ACOSCFDE in [18] It was reported that the performance of ACOSCFDE outperforms asymmetrically clipped optical OFDM (ACO OFDM) and OOK MMSE due to the high PAPR of ACOOFDM when the nonlinear characteristics of the LED are considered The performance of PAMSCFDE is compared with OFDM in [12] without consideration of the LED nonlinearity It was shown thatPAM SCFDE achieves higher performance gains when compared with OFDM at spectral efficiencies less than 3 bitssHz

Discrete Fourier transformation spread (DFTs) OFDM wasalso considered for LiFi as a SCM that has the benefits of anOFDM multicarrier system with lower PAPR [24] An extrapair of DFT and inverse discrete Fourier transformation (IDFT)operations are required to achieve DFTs OFDM Multiple independent streams of DFTs OFDM modulated waveforms areseparately transmitted through multiple LEDs in a single arrayThe performance of DFTs OFDM is reported to be better whencompared with DC biased optical OFDM (DCO OFDM) interms of both PAPR and bit error rate (BER) [24] A novel carrierless amplitude and phase (CAP) modulation was proposedfor Li Fi in [25] In order for CAP to suit the frequency response of LEDs the spectrum of CAP was divided into m subcarriers by the aid of finite impulse response (FIR) filter Al

3

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

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April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS32

though CAP is computationally complex it could offer highspectral efficiencies in bandlimited LiFi channel

4 Optical OFDMSingle carrier modulation techniques require a complex

equalization process when employed at high data rates In addition effects such as DC wandering and flickering interferenceof florescent lights may influence the system performance atthe lower frequency regions of the used bandwidth On the other hand multicarrier modulation techniques such as OFDMcan convert the frequency selective fading of the communication channel into a flat fading by employing the computationally efficient single tap equalizer In addition OFDM supportsadaptive power and bit loading which can adapt the channelutilization to the frequency response of the channel This canmaximize the system performance Supporting multiuser communication systems is an inherent advantage of OFDM whereeach user could be allocated certain subcarriers At the OFDMtransmitter the incoming bits are modulated into specific modulation formats such as M QAM The M QAM symbols areloaded afterwards into orthogonal subcarriers with subcarrierspacing equal to multiple of the symbol duration The parallelsymbols can then be multiplexed into a serial time domain output generally using inverse fast Fourier transformation (IFFT)The physical link of LiFi is achieved using offtheshelf optoelectronic devices such as LED and photodetectors (PD) Dueto the fact that these light sources produce an incoherent lightthe OFDM timedomain waveforms are used in LiFi to modulate the intensity of the LED source Therefore these waveforms are required to be both unipolar and real valued

Hermitian symmetry is generally imposed on the OFDM input frame to enforce the OFDM time domain signal output intothe real domain Different variants of optical OFDM were proposed to achieve a unipolar OFDM output DC bias is used inthe widely deployed DCOOFDM [26] to realize a unipolar timedomain OFDM output However OFDM signals have a highPAPR which makes it practically impossible to convert all ofthe signal samples into unipolar ones The OFDM timedomainwaveform can be approximated with a Normal distributionwhen the length of the input frame is greater than 64 The DCbias point would be dependent on the VL characteristic of theLED Zero level clipping of the remaining negative samples after the biasing would result in a clipping distortion that coulddeteriorate the system performance High DC bias would alsoincur some distortion as a result of the upper clipping of theOFDM waveform due to the V L characteristic of the idealLED The forward output current characteristic of an LED isshown in Fig 2 Predistortion is used to linearize the dynamicrange of the LED The LED input and output probability distribution function (PDF) of the OFDM modulation signal are alsoshown The dynamic range of the LED is between the turnonbias and the maximum allowed current points of the LED The

input signal is biased and the output signal is clipped for values outside the dynamic range The optimization of the DC biasing point was studied in [27]- [29] The additional dissipation of electrical power in DCOOFDM compared with bipolarOFDM increases as the modulation order increases This leadsto electrical and optical power inefficiency when DCOOFDMis used with high M QAM modulation orders Illumination isan essential part of VLC therefore the DCO OFDM opticalpower inefficiency can be justified for some VLC applicationsHowever when energy efficiency is required an alternativemodulation approach is required41 Inherent Unipolar Optical OFDM Techniques

Unipolar OFDM modulation schemes were mainly introduced to provide energy efficient optical OFDM alternatives toDCOOFDM These schemes include ACOOFDM [30] pulseamplitude modulated discrete multitone modulation (PAM DMT) [31] flipped OFDM (FlipOFDM) [32] and unipolar orthogonal frequency division multiplexing (UOFDM) [33] Theyexploit the OFDM inputoutput frame structure to produce aunipolar time domain waveform output However all of theseschemes have a reduced SE compared with DCOOFDM due tothe restrictions imposed on their frame structures In this section ACOOFDM PAMDMT and UOFDMFlipOFDM modulation schemes are discussed411 ACOOFDM

A real unipolar OFDM waveform can be achieved by exploiting the Fourier transformation properties on the frequency domain input OFDM frames The principle of ACOOFDM [30] isto skip the even subcarriers of an OFDM frame by only loading the odd subcarriers with useful information (Fig 3) Thiscreates a symmetry in the time domain OFDM signal which al

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

LED light emitting diode PDF probability distribution functionFigure 2 The forwardoutput current characteristic of an LED

I f

I out

LED transfer function

After predistortion

Dynamic rangeInput PDF

Output PDF

4

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

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April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 33

lows the distortionless clipping of the negative samples without the need of any DC biasing (Fig 4) Clipping of the negative values is distortionless since all of the distortion will onlyaffect the evenindexed subcarriers However skipping half ofthe subcarriers reduces the SE of ACOOFDM to half of that inDCOOFDM A penalty of 3 dB should applied to the signaltonoise ratio (SNR) of ACOOFDM when compared with bipolarOFDM since half of the signal power is lost due to clippingHermitian symmetry is also used to guarantee a real valuedACOOFDM output At the receiver after a fast Fourier transformation (FFT) is applied on the incoming frame only oddsubcarriers are considered412 PAMDMT

A real unipolar optical OFDM is realized in PAMDMT byexploiting the Fourier properties of imaginary signals The realcomponent of the subcarriers is not used in PAMDMT whichrestricts the modulation scheme used to MPAM (Fig 3) Byonly loading MPAM modulated symbols on the imaginary components of the subcarriers an antisymmetry in the time domain waveform of PAMDMT would be achieved (Fig 5) Thiswould facilitate the distortionless zero level clipping of PAMDMT waveform as all of the distortion would only affect the re

al component of the subcarriers Hermitian symmetry is alsoused to guarantee a real valued PAMDMT output PAMDMTis more attractive than ACO OFDM when bit loading techniques are considered as the PAMDMT performance can beoptimally adapted to the frequency response of the channelsince all of the subcarriers are used The SE of PAMDMT issimilar to that of DCOOFDM PAMDMT has a 3 dB fixedpenalty when compared with bipolar OFDM at an appropriateconstellation size as half of the power is also lost due to clipping At the receiver the imaginary part of the subcarriers isonly considered while the real part is ignored413 UOFDMFlipOFDM

The concept and performance of UOFDM and FlipOFDMis identical In this paper the term UOFDM is used howeverall discussion and analysis is applicable to both schemes Hermitian symmetry is applied on the incoming frame of MQAMsymbols The bipolar OFDM timedomain frame obtained afterwards is expanded into two timedomain frames in UOFDMwith similar sizes to the original OFDM frame (Fig 6) Thefirst frame is identical to the original frame while the secondis a flipped replica of the original frame A unipolar OFDMwaveform can be achieved by zero level clipping without theneed of any DC biasing At the receiver each second framewould be subtracted from the first frame of the same pair in order to reconstruct the original bipolar OFDM frame Thiswould double the noise at the receiver which leads to a 3 dBpenalty when compared with bipolar OFDM at equivalent constellation sizes The SE of UOFDM is half of the SE of DCOOFDM since two UOFDM frames are required to convey thesame information conveyed in a single DCOOFDM frame Thesingle tap equalizer can be used for UOFDM providing thatthe ISI effects on the first frame are identical to the ISI effectson the second frame414 Performance of Inherent Unipolar OFDM Techniques

The inherent unipolar OFDM schemes (ACO OFDM U OFDM and FlipOFDM) were introduced as power efficient alternatives to DCOOFDM However because two timedomainUOFDMFlipOFDM frames are required to convey the information contained in a single DCOOFDM frame and because

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 3 Subcarriers mapping of the input frames for DCOOFDMACOOFDM and PAMDMT Xi represents the M QAM symbol atthe i th subcarrier and Pi represents the M PAM symbol at the i thsubcarrier

ACOOFDM asymmetrically clipped optical OFDMDC direct current

DCOOFDM DCbiased optical OFDMPAMDMT pulseamplitudemodulated discrete multitone modulation

Figure 4 The timedomain ACOOFDM waveform

Figure 5 The timedomain PAMDMT waveform

DC X1 X2 X3 0 X 3 X 2 X 1

DCOOFDM Hermitian symmetry

0 X1 0 X3 0 X 3 0 X 1

ACOOFDM Hermitian symmetry

0 P1 P2 P3 0 P3 P2 P1

PAMDMT Hermitian symmetry

0 3 7

2

-2

0 n1051773 ACO(n)

0 1 3

2

-2

0 n

1051773 PAM(n) 1

-1

2Discrete time samples (s)

Discrete time samples (s)

5

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

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April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS34

half of the subcarriers are skipped in ACOOFDM the performance of M QAM DCOOFDM should be compared with theperformance of M2 QAM (ACOOFDM UOFDM and Flip OFDM) Additionally PAMDMT uses M PAM on the imaginary part of the subcarriers instead of MQAM Since the performance of M PAM is equivalent to the performance of M2 QAM the BER of PAMDMT is similar to that of the inherentunipolar schemes When compared with DCO OFDM at thesame SE the performance of all of the inherent unipolarOFDM techniques degrades as the constellation size of M QAM or M PAM increases For example the performance of1024QAM ACOOFDMUOFDMFlipOFDM and 32PAMPAMDMT would be required to be compared with the performance of 32QAM DCOOFDM

Improved receivers for all of the inherent unipolar OFDMtechniques were proposed in [33]-[41] Most of these improvedreceivers would either require a flat channel to operate or incur additional computational complexities Two main methodsare considered in the design of these improved receivers Inthe first method the timedomain symmetry can be exploitedat the receiver to achieve performance gains An amplitudecomparison between the symmetric received signal samplescan improve the receiver detection in flat fading channels atthe expense of increased computational complexity The second method is based on the frequency diversity The even subcarriers in ACOOFDM and the real part of the subcarriers inPAMDMT were exploited respectively to achieve improvedperformance at the receiver [33]-[41] The frequency diversitymethod can be used in the frequency selective channel however it has a higher computational complexity In addition it cannot be used for U OFDMFlip OFDM because both schemesare based on the timedomain processing of the OFDM framesBased on their statistical distribution the inherent unipolar optical OFDM waveforms utilize the lower part of the VL characteristic Therefore these schemes are suitable candidates for LiFi dimmable applications since they can operate with lower optical power dissipation Adaptive bit loading techniques werestudied for MCM techniques DCOOFDM and ACOOFDMand compared with SCFDE in [42] It was found that the per

formance of SC FDE is worse than ACO OFDM but better than DCOOFDM In addition SC FDE is less complex than DCO OFDM and ACOOFDM42 Hybrid OFDM Techniques

OFDM was modified in many studies totailor several specific aspects of the Li Fisystem parameters The natural spatial signal summing in the optical domain was proposed in [43] An array of multiple LEDs isused to transmit the OFDM signal so thatthe subcarriers are allocated to differentLEDs As the number of the LEDs in the ar

ray increases the PAPR of the electrical OFDM signals reduces When the number of subcarriers is equal to the number ofthe LEDs in the array the PAPR would reach its minimum value of 3 dB as the electrical signal would be an ideal sine waveThe spatial optical OFDM (SOOFDM) is reported to haveBER performance gains over DCOOFDM at high SNR due tothe reduced PAPR and the robustness against LED nonlinearities [43] Reverse polarity optical OFDM (RPOOFDM) wasproposed to allow a higher degree of illumination control in theOFDMbased LiFi systems [44] RPOOFDM combines a realvalued optical OFDM broadband technique with slow PWM toallow dimming The dynamic range of the LED is fully used inRPOOFDM to minimize any nonlinear distortion The RPOOFDM is reported to achieve higher performance gains compared with DCOOFDM at a large fraction of dimming rangeswithout limiting the data rate of the system RPOOFDM offersa practical solution for the illumination and dimming controlfor LiFi communication systems however the OFDM signal inRPOOFDM is based on unipolar OFDM This means that theSE of RPOOFDM is half of that of DCOOFDM As a resultthe power efficiency advantage over DCOOFDM starts to diminish as the SE increases In addition the PWM duty cycle isassumed to be known at the receiver which means that sideinformation should be sent before any transmission and this requires perfect synchronization between the transmitting and receiving ends A novel technique that combines ACOOFDM onthe odd subcarriers with DCOOFDM on the even subcarrierswas proposed in asymmetrically DC biased optical OFDM(ADOOFDM) [45] The clipping noise of the ACOOFDM fallsonly into the even subcarriers and can be estimated and canceled with a 3 dB penalty at the receiver The power allocationfor different constellation sizes between ACOOFDM and DCOOFDM streams in ADOOFDM was investigated in [15] Theoptical power efficiency of the optimal settings for ADO OFDM was better than ACOOFDM and DCOOFDM for different configurations Hybrid asymmetrical clipped OFDM (HACOOFDM) uses ACOOFDM on the odd subcarriers and PAMDMT on the even subcarriers to improve the SE of unipolarOFDM modulation techniques [46] The asymmetrical clipping

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 6 (a) Bipolar OFDM waveform (b) UOFDM waveform

0 5 10

5

0

X U[n]

n(b)

0 5

X Bip[n]

5

-5

0 n

(a)Discrete time samples (s) Discrete time samples (s)

+ -

6

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

of the ACOOFDM on the odd symbols would only distort theeven subcarriers At the receiver ACOOFDM symbols are demodulated first by only considering the odd subcarriers andthen remodulated to estimate the ACOOFDM distortion on theeven subcarriers This allows the PAMDMT symbols on theeven subcarrier to be demodulated without any distortion TheSE achieved in HACO OFDM is identical to that of DCO OFDM however PAMDMT uses M PAM modulation on halfof the subcarriers Equal power was allocated to ACOOFDMand PAMDMT As the performance of M2QAM is equivalentto the performance of MPAM the power requirements for bothACOOFDM and PAMDMT to achieve the same performanceis different The problem also appears when different modulation orders are used for both schemes Unequal power allocation for both schemes was investigated in [47] to guarantee thatthe performance of both schemes in HACO OFDM is equalAn improved but computationally complex receiver was alsoproposed in [47] based on the time domain symmetry of bothACOOFDM and PAMDMT

Polar OFDM (POFDM) is a new method to achieve the IMDD for OFDM [48] The main principle of POFDM is to convert the complex valued output of the IFFT from the Cartesiancoordinates into the polar coordinates Therefore the radialand angular coordinate can be sent in the first and secondhalves of the OFDM frame successively It avoids the use ofHermitian symmetry however it allocates the M QAM symbols into the even indexed subcarriers As a result P OFDMhas halfwave even symmetry which states that the first half ofthe complex valued timedomain frame is identical to the otherhalf Therefore it is sufficient to transmit the first half of theIFFT output As a result the SE is reduced to be identical tothat of DCOOFDM since only half of the subcarriers are usedThe performance of P OFDM was compared to that of ACOOFDM in [49] It was reported that P OFDM achieves betterBER performance gains than ACO OFDM under narrow dynamic ranges when optimal values for the power allocation ofthe radial and angular information are used Note that any ISIbetween the radial and angular samples may deteriorate thesystem performance therefore the system performance in frequency selective channels should be investigated Asymmetrical and symmetrical clipping optical OFDM (ASCO OFDM)was proposed in [50] for IMDD Li Fi systems The ACO OFDM is combined with symmetrical clipping optical OFDM(SCOOFDM) that uses the even subcarriers The clipping distortion of both ACOOFDM and SCOOFDM affects the evensubcarriers However the clipping distortion of ACO OFDMcan be estimated and canceled at the receiver The SCO OFDM clipping noise can be removed at the receiver using UOFDMFlip OFDM time domain processing techniques TheSE of ASCOOFDM is 75 of the SE of DCOOFDM ASCOOFDM was reported to have better symbol error rate (SER)compared with ADOOFDM since the ADOOFDM uses theDC bias for the even subcarriers FIR filtering technique

termed spectral factorization was used to create a unipolar optical OFDM signal [51] The amplitude of the subcarriers inspectral factorized optical OFDM (SFOOFDM) were chosen toform an autocorrelation sequence that was shown to be sufficient to guarantee a unipolar OFDM output The SFOOFDMwas reported to achieve 05 dB gain over ACO OFDM with30 PAPR reduction [51] The position modulation OFDM(PMOFDM) avoids the Hermitian symmetry and splits the realand imaginary components of the OFDM output into twobranches where a polarity separator is used to obtain the positive and negative samples of each branch [52] The four framescomposed of a real positive frame a real negative one an imaginary positive one and an imaginary negative one are transmitted as unipolar OFDM frames The SE is exactly similar to other inherent unipolar OFDM techniques discussed in section41 The performance of PMOFDM was reported to be identical to UOFDM in flat channels However it was reported tohave better BER performance when compared to ACOOFDMfor frequency selective channels [52]43 Superposition OFDM Techniques

Superposition OFDM based modulation techniques rely onthe fact that the SE of UOFDMFlipOFDM ACOOFDM andPAMDMT can be doubled by proper superimposing of multiple layers of OFDM waveforms Superposition modulation wasfirst introduced for OFDM based OWC and has led to enhanced UOFDM (eUOFDM) [53] The eUOFDM compensates for the spectral efficiency loss of UOFDM by superimposing multiple UOFDM streams so that the interstreaminterference is null The generation method of the first depth ineUOFDM is exactly similar to that in UOFDM Subsequentdepths can be generated by UOFDM modulators before eachunipolar OFDM frame is repeated 2d1 times and scaled by 12d1where d is the depth number At the receiver the informationconveyed in the first depth is demodulated and then remodulated to be subtracted from the overall received signal Then repeated frames which are equivalent at higher depths are recombined and the demodulation procedure continues the same asfor the stream at the first depth Afterwards the informationconveyed in latter depths is demodulated in a similar way TheSE gap between UOFDM and DCOOFDM can never be completely closed with eU OFDM as this would require a largenumber of information streams to be superimposed in the modulation signal Implementation issues such as latency computational complexity power penalty and memory requirementsput a practical limit on the maximum number of availabledepths The eUOFDM was generalized in the Generalized Enhanced Unipolar OFDM (GREENER OFDM) for configurations where arbitrary constellation sizes and arbitrary power allocations are used [54] As a result the SE gap between U OFDM and DCOOFDM can be closed completely with an appropriate selection of the constellation sizes in different information streams The symmetry in UOFDM lies in frames

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 35

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

7

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

whilst in ACOOFDM and PAMDMT it lies in subframesThe superposition concept has also been extended to other

unipolar OFDM techniques such as PAMDMT [55] and ACOOFDM [56]- [60] The enhanced asymmetrically clipped optical OFDM (eACO OFDM) [56] uses the symmetry of ACO OFDM subframes to allow multiple ACOOFDM streams to besuperimposed A similar concept was also proposed by Elgalaet al and Wang et al under the names of spectrally and energyefficient OFDM (SEEOFDM) [57] and layered asymmetricallyclipped optical OFDM (Layered ACOOFDM) [58] respectively The receiver proposed in SEEOFDM [57] results in SNRpenalty that could have been avoided by using the symmetryproperties of ACOOFDM streams The symmetry arrangementin Layered ACOOFDM [58] is described in the frequency domain however it is shown in [58 Fig2] that it takes place inthe time domain Recently an alternative method to achievesuperposition modulation based on ACOOFDM was proposedby Kozu et al [59] for two ACOOFDM streams and Lawery[60] for Layered ACO OFDM This is similar in principle tothe solutions in [56]- [58] however the superposition is performed in the frequency domain which results in simpler system design The concept of eACO OFDM was generalized toclose the SE gap between ACOOFDM and DCOOFDM Thegeneration of eACOOFDM signal starts at the first depth withan ACOOFDM modulator Additional depths are generated ina similar way to the first depth but with an OFDM framelength equal to half of the previous depth frames Similar to eUOFDM all of the generated frames are repeated 2dminus1 times andappropriately scaled The demodulation process at the receiveris applied in a similar way as the eUOFDM The informationat Depth1 can be recovered directly as in conventional ACOOFDM because all of the inter stream interference falls intothe evenindexed subcarriers After the first stream is decodedthe information can be remodulated again and subtracted fromthe overall received signal Then the frames that are equivalent can be recombined and the demodulation procedure continues as for the stream at first depth

The enhanced pulse amplitude modulated discrete multi tone (ePAMDMT) [55] demonstrates that superposition modulation can also be utilized when the antisymmetry of PAM DMT waveforms is used Analogous to eUOFDM and eACOOFDM unique timedomain structures are also present in PAMDMT If the interference over a single PAMDMT frame possesses a Hermitian symmetry in the timedomain its frequencyprofile falls on the real component of the subcarriers Hencethe interference is completely orthogonal to the useful information which is encoded in imaginary symbols of the PAMDMTframes The concept of superposition modulation was extendedto ePAMDMT for an arbitrary modulation order and an arbitrary power allocation at each depth [55] The theoretical BERanalysis of eACOOFDM is similar to the analysis of GREENEROFDM therefore the optimal modulation sizes and scalingfactors are identical This is an expected result because the

performance of their unipolar OFDM forms ACOOFDM and UOFDM is also similar The ePAMDMT is less energy efficientthan GREENER OFDM and eACO OFDM because ePAMDMT has 3 dB loss in each depth demodulation process andthe optimal configurations of ePAM DMT are suboptimal asthe non squared M QAM BER performance can never beachieved using the M PAM modulation scheme The ePAMDMT is more energy efficient than DCOOFDM in terms of theelectrical SNR at SE values above 1 bitsHz In terms of theoptical SNR the ePAMDMT is less energy efficient than DCOOFDM for all of the presented values Higher optical energydissipation is a desirable property for illumination based LiFiapplications but it is considered as a disadvantage for dimmablebased LiFi applications However GREENEROFDM andeACOOFDM are suitable candidates for dimmablebased LiFi applications due to their optical SNR performance

5 Other MultiCarrier ModulationTechniquesOFDM has been mainly studied in the context of LiFi chan

nels based on FFT Other transformations such as discreteHartley transformation (DHT) [61] wavelet packet divisionmultiplexing (WPDM) [62] and Hadamard coded modulation(HCM) [63] have also been considered for Li Fi channels Amulticarrier IMDD system based on DHT was proposed in[61] It was shown that DHT output can be real when an inputframe of real modulated symbols such as binary phase shiftkeying (BPSK) and M PAM is used Similar to DCOOFDMand ACOOFDM DCbiasing and asymmetrical clipping canalso be used to achieve unipolar output in DHTbased multicarrier modulation technique As a major advantage over FFTbased conventional OFDM the DHTbased multicarrier modulation does not require any Hermitian symmetry However thisfails to improve the SE as real modulated symbols such as MPAM are used in DHTbased multicarrier modulation WPDMuses orthogonal wavelet packet functions for symbol modulation where the basis functions are wavelet packet functionswith finite length It was reported that the performance of WPDM is better than that of OFDM in terms of the spectral andpower efficiencies when LED nonlinear distortion and channeldispersion are taken into account [62] The high illuminationlevel of OFDM Li Fi systems require higher optical powerwhich may result in clipping due to the peak power constraintof the VL transfer function of the LED (Fig 2) HCM was proposed for multicarrier modulation LiFi as a solution to the limitation of OFDM modulation at higher illumination levels Thetechnique is based on fast Walsh Hadamard transformation(FWHT) as an alternative to the FFT HCM is reported toachieve higher performance gains when compared with ACOOFDM and DCO OFDM at higher illumination levels [63]However the performance improvement over RPO OFDM ismodest An alternative variant of HCM termed DC reduced

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS36

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

8

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 4: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

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though CAP is computationally complex it could offer highspectral efficiencies in bandlimited LiFi channel

4 Optical OFDMSingle carrier modulation techniques require a complex

equalization process when employed at high data rates In addition effects such as DC wandering and flickering interferenceof florescent lights may influence the system performance atthe lower frequency regions of the used bandwidth On the other hand multicarrier modulation techniques such as OFDMcan convert the frequency selective fading of the communication channel into a flat fading by employing the computationally efficient single tap equalizer In addition OFDM supportsadaptive power and bit loading which can adapt the channelutilization to the frequency response of the channel This canmaximize the system performance Supporting multiuser communication systems is an inherent advantage of OFDM whereeach user could be allocated certain subcarriers At the OFDMtransmitter the incoming bits are modulated into specific modulation formats such as M QAM The M QAM symbols areloaded afterwards into orthogonal subcarriers with subcarrierspacing equal to multiple of the symbol duration The parallelsymbols can then be multiplexed into a serial time domain output generally using inverse fast Fourier transformation (IFFT)The physical link of LiFi is achieved using offtheshelf optoelectronic devices such as LED and photodetectors (PD) Dueto the fact that these light sources produce an incoherent lightthe OFDM timedomain waveforms are used in LiFi to modulate the intensity of the LED source Therefore these waveforms are required to be both unipolar and real valued

Hermitian symmetry is generally imposed on the OFDM input frame to enforce the OFDM time domain signal output intothe real domain Different variants of optical OFDM were proposed to achieve a unipolar OFDM output DC bias is used inthe widely deployed DCOOFDM [26] to realize a unipolar timedomain OFDM output However OFDM signals have a highPAPR which makes it practically impossible to convert all ofthe signal samples into unipolar ones The OFDM timedomainwaveform can be approximated with a Normal distributionwhen the length of the input frame is greater than 64 The DCbias point would be dependent on the VL characteristic of theLED Zero level clipping of the remaining negative samples after the biasing would result in a clipping distortion that coulddeteriorate the system performance High DC bias would alsoincur some distortion as a result of the upper clipping of theOFDM waveform due to the V L characteristic of the idealLED The forward output current characteristic of an LED isshown in Fig 2 Predistortion is used to linearize the dynamicrange of the LED The LED input and output probability distribution function (PDF) of the OFDM modulation signal are alsoshown The dynamic range of the LED is between the turnonbias and the maximum allowed current points of the LED The

input signal is biased and the output signal is clipped for values outside the dynamic range The optimization of the DC biasing point was studied in [27]- [29] The additional dissipation of electrical power in DCOOFDM compared with bipolarOFDM increases as the modulation order increases This leadsto electrical and optical power inefficiency when DCOOFDMis used with high M QAM modulation orders Illumination isan essential part of VLC therefore the DCO OFDM opticalpower inefficiency can be justified for some VLC applicationsHowever when energy efficiency is required an alternativemodulation approach is required41 Inherent Unipolar Optical OFDM Techniques

Unipolar OFDM modulation schemes were mainly introduced to provide energy efficient optical OFDM alternatives toDCOOFDM These schemes include ACOOFDM [30] pulseamplitude modulated discrete multitone modulation (PAM DMT) [31] flipped OFDM (FlipOFDM) [32] and unipolar orthogonal frequency division multiplexing (UOFDM) [33] Theyexploit the OFDM inputoutput frame structure to produce aunipolar time domain waveform output However all of theseschemes have a reduced SE compared with DCOOFDM due tothe restrictions imposed on their frame structures In this section ACOOFDM PAMDMT and UOFDMFlipOFDM modulation schemes are discussed411 ACOOFDM

A real unipolar OFDM waveform can be achieved by exploiting the Fourier transformation properties on the frequency domain input OFDM frames The principle of ACOOFDM [30] isto skip the even subcarriers of an OFDM frame by only loading the odd subcarriers with useful information (Fig 3) Thiscreates a symmetry in the time domain OFDM signal which al

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

LED light emitting diode PDF probability distribution functionFigure 2 The forwardoutput current characteristic of an LED

I f

I out

LED transfer function

After predistortion

Dynamic rangeInput PDF

Output PDF

4

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April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 33

lows the distortionless clipping of the negative samples without the need of any DC biasing (Fig 4) Clipping of the negative values is distortionless since all of the distortion will onlyaffect the evenindexed subcarriers However skipping half ofthe subcarriers reduces the SE of ACOOFDM to half of that inDCOOFDM A penalty of 3 dB should applied to the signaltonoise ratio (SNR) of ACOOFDM when compared with bipolarOFDM since half of the signal power is lost due to clippingHermitian symmetry is also used to guarantee a real valuedACOOFDM output At the receiver after a fast Fourier transformation (FFT) is applied on the incoming frame only oddsubcarriers are considered412 PAMDMT

A real unipolar optical OFDM is realized in PAMDMT byexploiting the Fourier properties of imaginary signals The realcomponent of the subcarriers is not used in PAMDMT whichrestricts the modulation scheme used to MPAM (Fig 3) Byonly loading MPAM modulated symbols on the imaginary components of the subcarriers an antisymmetry in the time domain waveform of PAMDMT would be achieved (Fig 5) Thiswould facilitate the distortionless zero level clipping of PAMDMT waveform as all of the distortion would only affect the re

al component of the subcarriers Hermitian symmetry is alsoused to guarantee a real valued PAMDMT output PAMDMTis more attractive than ACO OFDM when bit loading techniques are considered as the PAMDMT performance can beoptimally adapted to the frequency response of the channelsince all of the subcarriers are used The SE of PAMDMT issimilar to that of DCOOFDM PAMDMT has a 3 dB fixedpenalty when compared with bipolar OFDM at an appropriateconstellation size as half of the power is also lost due to clipping At the receiver the imaginary part of the subcarriers isonly considered while the real part is ignored413 UOFDMFlipOFDM

The concept and performance of UOFDM and FlipOFDMis identical In this paper the term UOFDM is used howeverall discussion and analysis is applicable to both schemes Hermitian symmetry is applied on the incoming frame of MQAMsymbols The bipolar OFDM timedomain frame obtained afterwards is expanded into two timedomain frames in UOFDMwith similar sizes to the original OFDM frame (Fig 6) Thefirst frame is identical to the original frame while the secondis a flipped replica of the original frame A unipolar OFDMwaveform can be achieved by zero level clipping without theneed of any DC biasing At the receiver each second framewould be subtracted from the first frame of the same pair in order to reconstruct the original bipolar OFDM frame Thiswould double the noise at the receiver which leads to a 3 dBpenalty when compared with bipolar OFDM at equivalent constellation sizes The SE of UOFDM is half of the SE of DCOOFDM since two UOFDM frames are required to convey thesame information conveyed in a single DCOOFDM frame Thesingle tap equalizer can be used for UOFDM providing thatthe ISI effects on the first frame are identical to the ISI effectson the second frame414 Performance of Inherent Unipolar OFDM Techniques

The inherent unipolar OFDM schemes (ACO OFDM U OFDM and FlipOFDM) were introduced as power efficient alternatives to DCOOFDM However because two timedomainUOFDMFlipOFDM frames are required to convey the information contained in a single DCOOFDM frame and because

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 3 Subcarriers mapping of the input frames for DCOOFDMACOOFDM and PAMDMT Xi represents the M QAM symbol atthe i th subcarrier and Pi represents the M PAM symbol at the i thsubcarrier

ACOOFDM asymmetrically clipped optical OFDMDC direct current

DCOOFDM DCbiased optical OFDMPAMDMT pulseamplitudemodulated discrete multitone modulation

Figure 4 The timedomain ACOOFDM waveform

Figure 5 The timedomain PAMDMT waveform

DC X1 X2 X3 0 X 3 X 2 X 1

DCOOFDM Hermitian symmetry

0 X1 0 X3 0 X 3 0 X 1

ACOOFDM Hermitian symmetry

0 P1 P2 P3 0 P3 P2 P1

PAMDMT Hermitian symmetry

0 3 7

2

-2

0 n1051773 ACO(n)

0 1 3

2

-2

0 n

1051773 PAM(n) 1

-1

2Discrete time samples (s)

Discrete time samples (s)

5

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half of the subcarriers are skipped in ACOOFDM the performance of M QAM DCOOFDM should be compared with theperformance of M2 QAM (ACOOFDM UOFDM and Flip OFDM) Additionally PAMDMT uses M PAM on the imaginary part of the subcarriers instead of MQAM Since the performance of M PAM is equivalent to the performance of M2 QAM the BER of PAMDMT is similar to that of the inherentunipolar schemes When compared with DCO OFDM at thesame SE the performance of all of the inherent unipolarOFDM techniques degrades as the constellation size of M QAM or M PAM increases For example the performance of1024QAM ACOOFDMUOFDMFlipOFDM and 32PAMPAMDMT would be required to be compared with the performance of 32QAM DCOOFDM

Improved receivers for all of the inherent unipolar OFDMtechniques were proposed in [33]-[41] Most of these improvedreceivers would either require a flat channel to operate or incur additional computational complexities Two main methodsare considered in the design of these improved receivers Inthe first method the timedomain symmetry can be exploitedat the receiver to achieve performance gains An amplitudecomparison between the symmetric received signal samplescan improve the receiver detection in flat fading channels atthe expense of increased computational complexity The second method is based on the frequency diversity The even subcarriers in ACOOFDM and the real part of the subcarriers inPAMDMT were exploited respectively to achieve improvedperformance at the receiver [33]-[41] The frequency diversitymethod can be used in the frequency selective channel however it has a higher computational complexity In addition it cannot be used for U OFDMFlip OFDM because both schemesare based on the timedomain processing of the OFDM framesBased on their statistical distribution the inherent unipolar optical OFDM waveforms utilize the lower part of the VL characteristic Therefore these schemes are suitable candidates for LiFi dimmable applications since they can operate with lower optical power dissipation Adaptive bit loading techniques werestudied for MCM techniques DCOOFDM and ACOOFDMand compared with SCFDE in [42] It was found that the per

formance of SC FDE is worse than ACO OFDM but better than DCOOFDM In addition SC FDE is less complex than DCO OFDM and ACOOFDM42 Hybrid OFDM Techniques

OFDM was modified in many studies totailor several specific aspects of the Li Fisystem parameters The natural spatial signal summing in the optical domain was proposed in [43] An array of multiple LEDs isused to transmit the OFDM signal so thatthe subcarriers are allocated to differentLEDs As the number of the LEDs in the ar

ray increases the PAPR of the electrical OFDM signals reduces When the number of subcarriers is equal to the number ofthe LEDs in the array the PAPR would reach its minimum value of 3 dB as the electrical signal would be an ideal sine waveThe spatial optical OFDM (SOOFDM) is reported to haveBER performance gains over DCOOFDM at high SNR due tothe reduced PAPR and the robustness against LED nonlinearities [43] Reverse polarity optical OFDM (RPOOFDM) wasproposed to allow a higher degree of illumination control in theOFDMbased LiFi systems [44] RPOOFDM combines a realvalued optical OFDM broadband technique with slow PWM toallow dimming The dynamic range of the LED is fully used inRPOOFDM to minimize any nonlinear distortion The RPOOFDM is reported to achieve higher performance gains compared with DCOOFDM at a large fraction of dimming rangeswithout limiting the data rate of the system RPOOFDM offersa practical solution for the illumination and dimming controlfor LiFi communication systems however the OFDM signal inRPOOFDM is based on unipolar OFDM This means that theSE of RPOOFDM is half of that of DCOOFDM As a resultthe power efficiency advantage over DCOOFDM starts to diminish as the SE increases In addition the PWM duty cycle isassumed to be known at the receiver which means that sideinformation should be sent before any transmission and this requires perfect synchronization between the transmitting and receiving ends A novel technique that combines ACOOFDM onthe odd subcarriers with DCOOFDM on the even subcarrierswas proposed in asymmetrically DC biased optical OFDM(ADOOFDM) [45] The clipping noise of the ACOOFDM fallsonly into the even subcarriers and can be estimated and canceled with a 3 dB penalty at the receiver The power allocationfor different constellation sizes between ACOOFDM and DCOOFDM streams in ADOOFDM was investigated in [15] Theoptical power efficiency of the optimal settings for ADO OFDM was better than ACOOFDM and DCOOFDM for different configurations Hybrid asymmetrical clipped OFDM (HACOOFDM) uses ACOOFDM on the odd subcarriers and PAMDMT on the even subcarriers to improve the SE of unipolarOFDM modulation techniques [46] The asymmetrical clipping

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 6 (a) Bipolar OFDM waveform (b) UOFDM waveform

0 5 10

5

0

X U[n]

n(b)

0 5

X Bip[n]

5

-5

0 n

(a)Discrete time samples (s) Discrete time samples (s)

+ -

6

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

of the ACOOFDM on the odd symbols would only distort theeven subcarriers At the receiver ACOOFDM symbols are demodulated first by only considering the odd subcarriers andthen remodulated to estimate the ACOOFDM distortion on theeven subcarriers This allows the PAMDMT symbols on theeven subcarrier to be demodulated without any distortion TheSE achieved in HACO OFDM is identical to that of DCO OFDM however PAMDMT uses M PAM modulation on halfof the subcarriers Equal power was allocated to ACOOFDMand PAMDMT As the performance of M2QAM is equivalentto the performance of MPAM the power requirements for bothACOOFDM and PAMDMT to achieve the same performanceis different The problem also appears when different modulation orders are used for both schemes Unequal power allocation for both schemes was investigated in [47] to guarantee thatthe performance of both schemes in HACO OFDM is equalAn improved but computationally complex receiver was alsoproposed in [47] based on the time domain symmetry of bothACOOFDM and PAMDMT

Polar OFDM (POFDM) is a new method to achieve the IMDD for OFDM [48] The main principle of POFDM is to convert the complex valued output of the IFFT from the Cartesiancoordinates into the polar coordinates Therefore the radialand angular coordinate can be sent in the first and secondhalves of the OFDM frame successively It avoids the use ofHermitian symmetry however it allocates the M QAM symbols into the even indexed subcarriers As a result P OFDMhas halfwave even symmetry which states that the first half ofthe complex valued timedomain frame is identical to the otherhalf Therefore it is sufficient to transmit the first half of theIFFT output As a result the SE is reduced to be identical tothat of DCOOFDM since only half of the subcarriers are usedThe performance of P OFDM was compared to that of ACOOFDM in [49] It was reported that P OFDM achieves betterBER performance gains than ACO OFDM under narrow dynamic ranges when optimal values for the power allocation ofthe radial and angular information are used Note that any ISIbetween the radial and angular samples may deteriorate thesystem performance therefore the system performance in frequency selective channels should be investigated Asymmetrical and symmetrical clipping optical OFDM (ASCO OFDM)was proposed in [50] for IMDD Li Fi systems The ACO OFDM is combined with symmetrical clipping optical OFDM(SCOOFDM) that uses the even subcarriers The clipping distortion of both ACOOFDM and SCOOFDM affects the evensubcarriers However the clipping distortion of ACO OFDMcan be estimated and canceled at the receiver The SCO OFDM clipping noise can be removed at the receiver using UOFDMFlip OFDM time domain processing techniques TheSE of ASCOOFDM is 75 of the SE of DCOOFDM ASCOOFDM was reported to have better symbol error rate (SER)compared with ADOOFDM since the ADOOFDM uses theDC bias for the even subcarriers FIR filtering technique

termed spectral factorization was used to create a unipolar optical OFDM signal [51] The amplitude of the subcarriers inspectral factorized optical OFDM (SFOOFDM) were chosen toform an autocorrelation sequence that was shown to be sufficient to guarantee a unipolar OFDM output The SFOOFDMwas reported to achieve 05 dB gain over ACO OFDM with30 PAPR reduction [51] The position modulation OFDM(PMOFDM) avoids the Hermitian symmetry and splits the realand imaginary components of the OFDM output into twobranches where a polarity separator is used to obtain the positive and negative samples of each branch [52] The four framescomposed of a real positive frame a real negative one an imaginary positive one and an imaginary negative one are transmitted as unipolar OFDM frames The SE is exactly similar to other inherent unipolar OFDM techniques discussed in section41 The performance of PMOFDM was reported to be identical to UOFDM in flat channels However it was reported tohave better BER performance when compared to ACOOFDMfor frequency selective channels [52]43 Superposition OFDM Techniques

Superposition OFDM based modulation techniques rely onthe fact that the SE of UOFDMFlipOFDM ACOOFDM andPAMDMT can be doubled by proper superimposing of multiple layers of OFDM waveforms Superposition modulation wasfirst introduced for OFDM based OWC and has led to enhanced UOFDM (eUOFDM) [53] The eUOFDM compensates for the spectral efficiency loss of UOFDM by superimposing multiple UOFDM streams so that the interstreaminterference is null The generation method of the first depth ineUOFDM is exactly similar to that in UOFDM Subsequentdepths can be generated by UOFDM modulators before eachunipolar OFDM frame is repeated 2d1 times and scaled by 12d1where d is the depth number At the receiver the informationconveyed in the first depth is demodulated and then remodulated to be subtracted from the overall received signal Then repeated frames which are equivalent at higher depths are recombined and the demodulation procedure continues the same asfor the stream at the first depth Afterwards the informationconveyed in latter depths is demodulated in a similar way TheSE gap between UOFDM and DCOOFDM can never be completely closed with eU OFDM as this would require a largenumber of information streams to be superimposed in the modulation signal Implementation issues such as latency computational complexity power penalty and memory requirementsput a practical limit on the maximum number of availabledepths The eUOFDM was generalized in the Generalized Enhanced Unipolar OFDM (GREENER OFDM) for configurations where arbitrary constellation sizes and arbitrary power allocations are used [54] As a result the SE gap between U OFDM and DCOOFDM can be closed completely with an appropriate selection of the constellation sizes in different information streams The symmetry in UOFDM lies in frames

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April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 35

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

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DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

whilst in ACOOFDM and PAMDMT it lies in subframesThe superposition concept has also been extended to other

unipolar OFDM techniques such as PAMDMT [55] and ACOOFDM [56]- [60] The enhanced asymmetrically clipped optical OFDM (eACO OFDM) [56] uses the symmetry of ACO OFDM subframes to allow multiple ACOOFDM streams to besuperimposed A similar concept was also proposed by Elgalaet al and Wang et al under the names of spectrally and energyefficient OFDM (SEEOFDM) [57] and layered asymmetricallyclipped optical OFDM (Layered ACOOFDM) [58] respectively The receiver proposed in SEEOFDM [57] results in SNRpenalty that could have been avoided by using the symmetryproperties of ACOOFDM streams The symmetry arrangementin Layered ACOOFDM [58] is described in the frequency domain however it is shown in [58 Fig2] that it takes place inthe time domain Recently an alternative method to achievesuperposition modulation based on ACOOFDM was proposedby Kozu et al [59] for two ACOOFDM streams and Lawery[60] for Layered ACO OFDM This is similar in principle tothe solutions in [56]- [58] however the superposition is performed in the frequency domain which results in simpler system design The concept of eACO OFDM was generalized toclose the SE gap between ACOOFDM and DCOOFDM Thegeneration of eACOOFDM signal starts at the first depth withan ACOOFDM modulator Additional depths are generated ina similar way to the first depth but with an OFDM framelength equal to half of the previous depth frames Similar to eUOFDM all of the generated frames are repeated 2dminus1 times andappropriately scaled The demodulation process at the receiveris applied in a similar way as the eUOFDM The informationat Depth1 can be recovered directly as in conventional ACOOFDM because all of the inter stream interference falls intothe evenindexed subcarriers After the first stream is decodedthe information can be remodulated again and subtracted fromthe overall received signal Then the frames that are equivalent can be recombined and the demodulation procedure continues as for the stream at first depth

The enhanced pulse amplitude modulated discrete multi tone (ePAMDMT) [55] demonstrates that superposition modulation can also be utilized when the antisymmetry of PAM DMT waveforms is used Analogous to eUOFDM and eACOOFDM unique timedomain structures are also present in PAMDMT If the interference over a single PAMDMT frame possesses a Hermitian symmetry in the timedomain its frequencyprofile falls on the real component of the subcarriers Hencethe interference is completely orthogonal to the useful information which is encoded in imaginary symbols of the PAMDMTframes The concept of superposition modulation was extendedto ePAMDMT for an arbitrary modulation order and an arbitrary power allocation at each depth [55] The theoretical BERanalysis of eACOOFDM is similar to the analysis of GREENEROFDM therefore the optimal modulation sizes and scalingfactors are identical This is an expected result because the

performance of their unipolar OFDM forms ACOOFDM and UOFDM is also similar The ePAMDMT is less energy efficientthan GREENER OFDM and eACO OFDM because ePAMDMT has 3 dB loss in each depth demodulation process andthe optimal configurations of ePAM DMT are suboptimal asthe non squared M QAM BER performance can never beachieved using the M PAM modulation scheme The ePAMDMT is more energy efficient than DCOOFDM in terms of theelectrical SNR at SE values above 1 bitsHz In terms of theoptical SNR the ePAMDMT is less energy efficient than DCOOFDM for all of the presented values Higher optical energydissipation is a desirable property for illumination based LiFiapplications but it is considered as a disadvantage for dimmablebased LiFi applications However GREENEROFDM andeACOOFDM are suitable candidates for dimmablebased LiFi applications due to their optical SNR performance

5 Other MultiCarrier ModulationTechniquesOFDM has been mainly studied in the context of LiFi chan

nels based on FFT Other transformations such as discreteHartley transformation (DHT) [61] wavelet packet divisionmultiplexing (WPDM) [62] and Hadamard coded modulation(HCM) [63] have also been considered for Li Fi channels Amulticarrier IMDD system based on DHT was proposed in[61] It was shown that DHT output can be real when an inputframe of real modulated symbols such as binary phase shiftkeying (BPSK) and M PAM is used Similar to DCOOFDMand ACOOFDM DCbiasing and asymmetrical clipping canalso be used to achieve unipolar output in DHTbased multicarrier modulation technique As a major advantage over FFTbased conventional OFDM the DHTbased multicarrier modulation does not require any Hermitian symmetry However thisfails to improve the SE as real modulated symbols such as MPAM are used in DHTbased multicarrier modulation WPDMuses orthogonal wavelet packet functions for symbol modulation where the basis functions are wavelet packet functionswith finite length It was reported that the performance of WPDM is better than that of OFDM in terms of the spectral andpower efficiencies when LED nonlinear distortion and channeldispersion are taken into account [62] The high illuminationlevel of OFDM Li Fi systems require higher optical powerwhich may result in clipping due to the peak power constraintof the VL transfer function of the LED (Fig 2) HCM was proposed for multicarrier modulation LiFi as a solution to the limitation of OFDM modulation at higher illumination levels Thetechnique is based on fast Walsh Hadamard transformation(FWHT) as an alternative to the FFT HCM is reported toachieve higher performance gains when compared with ACOOFDM and DCO OFDM at higher illumination levels [63]However the performance improvement over RPO OFDM ismodest An alternative variant of HCM termed DC reduced

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April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS36

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

8

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

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April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 5: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 33

lows the distortionless clipping of the negative samples without the need of any DC biasing (Fig 4) Clipping of the negative values is distortionless since all of the distortion will onlyaffect the evenindexed subcarriers However skipping half ofthe subcarriers reduces the SE of ACOOFDM to half of that inDCOOFDM A penalty of 3 dB should applied to the signaltonoise ratio (SNR) of ACOOFDM when compared with bipolarOFDM since half of the signal power is lost due to clippingHermitian symmetry is also used to guarantee a real valuedACOOFDM output At the receiver after a fast Fourier transformation (FFT) is applied on the incoming frame only oddsubcarriers are considered412 PAMDMT

A real unipolar optical OFDM is realized in PAMDMT byexploiting the Fourier properties of imaginary signals The realcomponent of the subcarriers is not used in PAMDMT whichrestricts the modulation scheme used to MPAM (Fig 3) Byonly loading MPAM modulated symbols on the imaginary components of the subcarriers an antisymmetry in the time domain waveform of PAMDMT would be achieved (Fig 5) Thiswould facilitate the distortionless zero level clipping of PAMDMT waveform as all of the distortion would only affect the re

al component of the subcarriers Hermitian symmetry is alsoused to guarantee a real valued PAMDMT output PAMDMTis more attractive than ACO OFDM when bit loading techniques are considered as the PAMDMT performance can beoptimally adapted to the frequency response of the channelsince all of the subcarriers are used The SE of PAMDMT issimilar to that of DCOOFDM PAMDMT has a 3 dB fixedpenalty when compared with bipolar OFDM at an appropriateconstellation size as half of the power is also lost due to clipping At the receiver the imaginary part of the subcarriers isonly considered while the real part is ignored413 UOFDMFlipOFDM

The concept and performance of UOFDM and FlipOFDMis identical In this paper the term UOFDM is used howeverall discussion and analysis is applicable to both schemes Hermitian symmetry is applied on the incoming frame of MQAMsymbols The bipolar OFDM timedomain frame obtained afterwards is expanded into two timedomain frames in UOFDMwith similar sizes to the original OFDM frame (Fig 6) Thefirst frame is identical to the original frame while the secondis a flipped replica of the original frame A unipolar OFDMwaveform can be achieved by zero level clipping without theneed of any DC biasing At the receiver each second framewould be subtracted from the first frame of the same pair in order to reconstruct the original bipolar OFDM frame Thiswould double the noise at the receiver which leads to a 3 dBpenalty when compared with bipolar OFDM at equivalent constellation sizes The SE of UOFDM is half of the SE of DCOOFDM since two UOFDM frames are required to convey thesame information conveyed in a single DCOOFDM frame Thesingle tap equalizer can be used for UOFDM providing thatthe ISI effects on the first frame are identical to the ISI effectson the second frame414 Performance of Inherent Unipolar OFDM Techniques

The inherent unipolar OFDM schemes (ACO OFDM U OFDM and FlipOFDM) were introduced as power efficient alternatives to DCOOFDM However because two timedomainUOFDMFlipOFDM frames are required to convey the information contained in a single DCOOFDM frame and because

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 3 Subcarriers mapping of the input frames for DCOOFDMACOOFDM and PAMDMT Xi represents the M QAM symbol atthe i th subcarrier and Pi represents the M PAM symbol at the i thsubcarrier

ACOOFDM asymmetrically clipped optical OFDMDC direct current

DCOOFDM DCbiased optical OFDMPAMDMT pulseamplitudemodulated discrete multitone modulation

Figure 4 The timedomain ACOOFDM waveform

Figure 5 The timedomain PAMDMT waveform

DC X1 X2 X3 0 X 3 X 2 X 1

DCOOFDM Hermitian symmetry

0 X1 0 X3 0 X 3 0 X 1

ACOOFDM Hermitian symmetry

0 P1 P2 P3 0 P3 P2 P1

PAMDMT Hermitian symmetry

0 3 7

2

-2

0 n1051773 ACO(n)

0 1 3

2

-2

0 n

1051773 PAM(n) 1

-1

2Discrete time samples (s)

Discrete time samples (s)

5

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS34

half of the subcarriers are skipped in ACOOFDM the performance of M QAM DCOOFDM should be compared with theperformance of M2 QAM (ACOOFDM UOFDM and Flip OFDM) Additionally PAMDMT uses M PAM on the imaginary part of the subcarriers instead of MQAM Since the performance of M PAM is equivalent to the performance of M2 QAM the BER of PAMDMT is similar to that of the inherentunipolar schemes When compared with DCO OFDM at thesame SE the performance of all of the inherent unipolarOFDM techniques degrades as the constellation size of M QAM or M PAM increases For example the performance of1024QAM ACOOFDMUOFDMFlipOFDM and 32PAMPAMDMT would be required to be compared with the performance of 32QAM DCOOFDM

Improved receivers for all of the inherent unipolar OFDMtechniques were proposed in [33]-[41] Most of these improvedreceivers would either require a flat channel to operate or incur additional computational complexities Two main methodsare considered in the design of these improved receivers Inthe first method the timedomain symmetry can be exploitedat the receiver to achieve performance gains An amplitudecomparison between the symmetric received signal samplescan improve the receiver detection in flat fading channels atthe expense of increased computational complexity The second method is based on the frequency diversity The even subcarriers in ACOOFDM and the real part of the subcarriers inPAMDMT were exploited respectively to achieve improvedperformance at the receiver [33]-[41] The frequency diversitymethod can be used in the frequency selective channel however it has a higher computational complexity In addition it cannot be used for U OFDMFlip OFDM because both schemesare based on the timedomain processing of the OFDM framesBased on their statistical distribution the inherent unipolar optical OFDM waveforms utilize the lower part of the VL characteristic Therefore these schemes are suitable candidates for LiFi dimmable applications since they can operate with lower optical power dissipation Adaptive bit loading techniques werestudied for MCM techniques DCOOFDM and ACOOFDMand compared with SCFDE in [42] It was found that the per

formance of SC FDE is worse than ACO OFDM but better than DCOOFDM In addition SC FDE is less complex than DCO OFDM and ACOOFDM42 Hybrid OFDM Techniques

OFDM was modified in many studies totailor several specific aspects of the Li Fisystem parameters The natural spatial signal summing in the optical domain was proposed in [43] An array of multiple LEDs isused to transmit the OFDM signal so thatthe subcarriers are allocated to differentLEDs As the number of the LEDs in the ar

ray increases the PAPR of the electrical OFDM signals reduces When the number of subcarriers is equal to the number ofthe LEDs in the array the PAPR would reach its minimum value of 3 dB as the electrical signal would be an ideal sine waveThe spatial optical OFDM (SOOFDM) is reported to haveBER performance gains over DCOOFDM at high SNR due tothe reduced PAPR and the robustness against LED nonlinearities [43] Reverse polarity optical OFDM (RPOOFDM) wasproposed to allow a higher degree of illumination control in theOFDMbased LiFi systems [44] RPOOFDM combines a realvalued optical OFDM broadband technique with slow PWM toallow dimming The dynamic range of the LED is fully used inRPOOFDM to minimize any nonlinear distortion The RPOOFDM is reported to achieve higher performance gains compared with DCOOFDM at a large fraction of dimming rangeswithout limiting the data rate of the system RPOOFDM offersa practical solution for the illumination and dimming controlfor LiFi communication systems however the OFDM signal inRPOOFDM is based on unipolar OFDM This means that theSE of RPOOFDM is half of that of DCOOFDM As a resultthe power efficiency advantage over DCOOFDM starts to diminish as the SE increases In addition the PWM duty cycle isassumed to be known at the receiver which means that sideinformation should be sent before any transmission and this requires perfect synchronization between the transmitting and receiving ends A novel technique that combines ACOOFDM onthe odd subcarriers with DCOOFDM on the even subcarrierswas proposed in asymmetrically DC biased optical OFDM(ADOOFDM) [45] The clipping noise of the ACOOFDM fallsonly into the even subcarriers and can be estimated and canceled with a 3 dB penalty at the receiver The power allocationfor different constellation sizes between ACOOFDM and DCOOFDM streams in ADOOFDM was investigated in [15] Theoptical power efficiency of the optimal settings for ADO OFDM was better than ACOOFDM and DCOOFDM for different configurations Hybrid asymmetrical clipped OFDM (HACOOFDM) uses ACOOFDM on the odd subcarriers and PAMDMT on the even subcarriers to improve the SE of unipolarOFDM modulation techniques [46] The asymmetrical clipping

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 6 (a) Bipolar OFDM waveform (b) UOFDM waveform

0 5 10

5

0

X U[n]

n(b)

0 5

X Bip[n]

5

-5

0 n

(a)Discrete time samples (s) Discrete time samples (s)

+ -

6

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

of the ACOOFDM on the odd symbols would only distort theeven subcarriers At the receiver ACOOFDM symbols are demodulated first by only considering the odd subcarriers andthen remodulated to estimate the ACOOFDM distortion on theeven subcarriers This allows the PAMDMT symbols on theeven subcarrier to be demodulated without any distortion TheSE achieved in HACO OFDM is identical to that of DCO OFDM however PAMDMT uses M PAM modulation on halfof the subcarriers Equal power was allocated to ACOOFDMand PAMDMT As the performance of M2QAM is equivalentto the performance of MPAM the power requirements for bothACOOFDM and PAMDMT to achieve the same performanceis different The problem also appears when different modulation orders are used for both schemes Unequal power allocation for both schemes was investigated in [47] to guarantee thatthe performance of both schemes in HACO OFDM is equalAn improved but computationally complex receiver was alsoproposed in [47] based on the time domain symmetry of bothACOOFDM and PAMDMT

Polar OFDM (POFDM) is a new method to achieve the IMDD for OFDM [48] The main principle of POFDM is to convert the complex valued output of the IFFT from the Cartesiancoordinates into the polar coordinates Therefore the radialand angular coordinate can be sent in the first and secondhalves of the OFDM frame successively It avoids the use ofHermitian symmetry however it allocates the M QAM symbols into the even indexed subcarriers As a result P OFDMhas halfwave even symmetry which states that the first half ofthe complex valued timedomain frame is identical to the otherhalf Therefore it is sufficient to transmit the first half of theIFFT output As a result the SE is reduced to be identical tothat of DCOOFDM since only half of the subcarriers are usedThe performance of P OFDM was compared to that of ACOOFDM in [49] It was reported that P OFDM achieves betterBER performance gains than ACO OFDM under narrow dynamic ranges when optimal values for the power allocation ofthe radial and angular information are used Note that any ISIbetween the radial and angular samples may deteriorate thesystem performance therefore the system performance in frequency selective channels should be investigated Asymmetrical and symmetrical clipping optical OFDM (ASCO OFDM)was proposed in [50] for IMDD Li Fi systems The ACO OFDM is combined with symmetrical clipping optical OFDM(SCOOFDM) that uses the even subcarriers The clipping distortion of both ACOOFDM and SCOOFDM affects the evensubcarriers However the clipping distortion of ACO OFDMcan be estimated and canceled at the receiver The SCO OFDM clipping noise can be removed at the receiver using UOFDMFlip OFDM time domain processing techniques TheSE of ASCOOFDM is 75 of the SE of DCOOFDM ASCOOFDM was reported to have better symbol error rate (SER)compared with ADOOFDM since the ADOOFDM uses theDC bias for the even subcarriers FIR filtering technique

termed spectral factorization was used to create a unipolar optical OFDM signal [51] The amplitude of the subcarriers inspectral factorized optical OFDM (SFOOFDM) were chosen toform an autocorrelation sequence that was shown to be sufficient to guarantee a unipolar OFDM output The SFOOFDMwas reported to achieve 05 dB gain over ACO OFDM with30 PAPR reduction [51] The position modulation OFDM(PMOFDM) avoids the Hermitian symmetry and splits the realand imaginary components of the OFDM output into twobranches where a polarity separator is used to obtain the positive and negative samples of each branch [52] The four framescomposed of a real positive frame a real negative one an imaginary positive one and an imaginary negative one are transmitted as unipolar OFDM frames The SE is exactly similar to other inherent unipolar OFDM techniques discussed in section41 The performance of PMOFDM was reported to be identical to UOFDM in flat channels However it was reported tohave better BER performance when compared to ACOOFDMfor frequency selective channels [52]43 Superposition OFDM Techniques

Superposition OFDM based modulation techniques rely onthe fact that the SE of UOFDMFlipOFDM ACOOFDM andPAMDMT can be doubled by proper superimposing of multiple layers of OFDM waveforms Superposition modulation wasfirst introduced for OFDM based OWC and has led to enhanced UOFDM (eUOFDM) [53] The eUOFDM compensates for the spectral efficiency loss of UOFDM by superimposing multiple UOFDM streams so that the interstreaminterference is null The generation method of the first depth ineUOFDM is exactly similar to that in UOFDM Subsequentdepths can be generated by UOFDM modulators before eachunipolar OFDM frame is repeated 2d1 times and scaled by 12d1where d is the depth number At the receiver the informationconveyed in the first depth is demodulated and then remodulated to be subtracted from the overall received signal Then repeated frames which are equivalent at higher depths are recombined and the demodulation procedure continues the same asfor the stream at the first depth Afterwards the informationconveyed in latter depths is demodulated in a similar way TheSE gap between UOFDM and DCOOFDM can never be completely closed with eU OFDM as this would require a largenumber of information streams to be superimposed in the modulation signal Implementation issues such as latency computational complexity power penalty and memory requirementsput a practical limit on the maximum number of availabledepths The eUOFDM was generalized in the Generalized Enhanced Unipolar OFDM (GREENER OFDM) for configurations where arbitrary constellation sizes and arbitrary power allocations are used [54] As a result the SE gap between U OFDM and DCOOFDM can be closed completely with an appropriate selection of the constellation sizes in different information streams The symmetry in UOFDM lies in frames

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 35

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

7

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

whilst in ACOOFDM and PAMDMT it lies in subframesThe superposition concept has also been extended to other

unipolar OFDM techniques such as PAMDMT [55] and ACOOFDM [56]- [60] The enhanced asymmetrically clipped optical OFDM (eACO OFDM) [56] uses the symmetry of ACO OFDM subframes to allow multiple ACOOFDM streams to besuperimposed A similar concept was also proposed by Elgalaet al and Wang et al under the names of spectrally and energyefficient OFDM (SEEOFDM) [57] and layered asymmetricallyclipped optical OFDM (Layered ACOOFDM) [58] respectively The receiver proposed in SEEOFDM [57] results in SNRpenalty that could have been avoided by using the symmetryproperties of ACOOFDM streams The symmetry arrangementin Layered ACOOFDM [58] is described in the frequency domain however it is shown in [58 Fig2] that it takes place inthe time domain Recently an alternative method to achievesuperposition modulation based on ACOOFDM was proposedby Kozu et al [59] for two ACOOFDM streams and Lawery[60] for Layered ACO OFDM This is similar in principle tothe solutions in [56]- [58] however the superposition is performed in the frequency domain which results in simpler system design The concept of eACO OFDM was generalized toclose the SE gap between ACOOFDM and DCOOFDM Thegeneration of eACOOFDM signal starts at the first depth withan ACOOFDM modulator Additional depths are generated ina similar way to the first depth but with an OFDM framelength equal to half of the previous depth frames Similar to eUOFDM all of the generated frames are repeated 2dminus1 times andappropriately scaled The demodulation process at the receiveris applied in a similar way as the eUOFDM The informationat Depth1 can be recovered directly as in conventional ACOOFDM because all of the inter stream interference falls intothe evenindexed subcarriers After the first stream is decodedthe information can be remodulated again and subtracted fromthe overall received signal Then the frames that are equivalent can be recombined and the demodulation procedure continues as for the stream at first depth

The enhanced pulse amplitude modulated discrete multi tone (ePAMDMT) [55] demonstrates that superposition modulation can also be utilized when the antisymmetry of PAM DMT waveforms is used Analogous to eUOFDM and eACOOFDM unique timedomain structures are also present in PAMDMT If the interference over a single PAMDMT frame possesses a Hermitian symmetry in the timedomain its frequencyprofile falls on the real component of the subcarriers Hencethe interference is completely orthogonal to the useful information which is encoded in imaginary symbols of the PAMDMTframes The concept of superposition modulation was extendedto ePAMDMT for an arbitrary modulation order and an arbitrary power allocation at each depth [55] The theoretical BERanalysis of eACOOFDM is similar to the analysis of GREENEROFDM therefore the optimal modulation sizes and scalingfactors are identical This is an expected result because the

performance of their unipolar OFDM forms ACOOFDM and UOFDM is also similar The ePAMDMT is less energy efficientthan GREENER OFDM and eACO OFDM because ePAMDMT has 3 dB loss in each depth demodulation process andthe optimal configurations of ePAM DMT are suboptimal asthe non squared M QAM BER performance can never beachieved using the M PAM modulation scheme The ePAMDMT is more energy efficient than DCOOFDM in terms of theelectrical SNR at SE values above 1 bitsHz In terms of theoptical SNR the ePAMDMT is less energy efficient than DCOOFDM for all of the presented values Higher optical energydissipation is a desirable property for illumination based LiFiapplications but it is considered as a disadvantage for dimmablebased LiFi applications However GREENEROFDM andeACOOFDM are suitable candidates for dimmablebased LiFi applications due to their optical SNR performance

5 Other MultiCarrier ModulationTechniquesOFDM has been mainly studied in the context of LiFi chan

nels based on FFT Other transformations such as discreteHartley transformation (DHT) [61] wavelet packet divisionmultiplexing (WPDM) [62] and Hadamard coded modulation(HCM) [63] have also been considered for Li Fi channels Amulticarrier IMDD system based on DHT was proposed in[61] It was shown that DHT output can be real when an inputframe of real modulated symbols such as binary phase shiftkeying (BPSK) and M PAM is used Similar to DCOOFDMand ACOOFDM DCbiasing and asymmetrical clipping canalso be used to achieve unipolar output in DHTbased multicarrier modulation technique As a major advantage over FFTbased conventional OFDM the DHTbased multicarrier modulation does not require any Hermitian symmetry However thisfails to improve the SE as real modulated symbols such as MPAM are used in DHTbased multicarrier modulation WPDMuses orthogonal wavelet packet functions for symbol modulation where the basis functions are wavelet packet functionswith finite length It was reported that the performance of WPDM is better than that of OFDM in terms of the spectral andpower efficiencies when LED nonlinear distortion and channeldispersion are taken into account [62] The high illuminationlevel of OFDM Li Fi systems require higher optical powerwhich may result in clipping due to the peak power constraintof the VL transfer function of the LED (Fig 2) HCM was proposed for multicarrier modulation LiFi as a solution to the limitation of OFDM modulation at higher illumination levels Thetechnique is based on fast Walsh Hadamard transformation(FWHT) as an alternative to the FFT HCM is reported toachieve higher performance gains when compared with ACOOFDM and DCO OFDM at higher illumination levels [63]However the performance improvement over RPO OFDM ismodest An alternative variant of HCM termed DC reduced

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS36

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

8

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 6: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS34

half of the subcarriers are skipped in ACOOFDM the performance of M QAM DCOOFDM should be compared with theperformance of M2 QAM (ACOOFDM UOFDM and Flip OFDM) Additionally PAMDMT uses M PAM on the imaginary part of the subcarriers instead of MQAM Since the performance of M PAM is equivalent to the performance of M2 QAM the BER of PAMDMT is similar to that of the inherentunipolar schemes When compared with DCO OFDM at thesame SE the performance of all of the inherent unipolarOFDM techniques degrades as the constellation size of M QAM or M PAM increases For example the performance of1024QAM ACOOFDMUOFDMFlipOFDM and 32PAMPAMDMT would be required to be compared with the performance of 32QAM DCOOFDM

Improved receivers for all of the inherent unipolar OFDMtechniques were proposed in [33]-[41] Most of these improvedreceivers would either require a flat channel to operate or incur additional computational complexities Two main methodsare considered in the design of these improved receivers Inthe first method the timedomain symmetry can be exploitedat the receiver to achieve performance gains An amplitudecomparison between the symmetric received signal samplescan improve the receiver detection in flat fading channels atthe expense of increased computational complexity The second method is based on the frequency diversity The even subcarriers in ACOOFDM and the real part of the subcarriers inPAMDMT were exploited respectively to achieve improvedperformance at the receiver [33]-[41] The frequency diversitymethod can be used in the frequency selective channel however it has a higher computational complexity In addition it cannot be used for U OFDMFlip OFDM because both schemesare based on the timedomain processing of the OFDM framesBased on their statistical distribution the inherent unipolar optical OFDM waveforms utilize the lower part of the VL characteristic Therefore these schemes are suitable candidates for LiFi dimmable applications since they can operate with lower optical power dissipation Adaptive bit loading techniques werestudied for MCM techniques DCOOFDM and ACOOFDMand compared with SCFDE in [42] It was found that the per

formance of SC FDE is worse than ACO OFDM but better than DCOOFDM In addition SC FDE is less complex than DCO OFDM and ACOOFDM42 Hybrid OFDM Techniques

OFDM was modified in many studies totailor several specific aspects of the Li Fisystem parameters The natural spatial signal summing in the optical domain was proposed in [43] An array of multiple LEDs isused to transmit the OFDM signal so thatthe subcarriers are allocated to differentLEDs As the number of the LEDs in the ar

ray increases the PAPR of the electrical OFDM signals reduces When the number of subcarriers is equal to the number ofthe LEDs in the array the PAPR would reach its minimum value of 3 dB as the electrical signal would be an ideal sine waveThe spatial optical OFDM (SOOFDM) is reported to haveBER performance gains over DCOOFDM at high SNR due tothe reduced PAPR and the robustness against LED nonlinearities [43] Reverse polarity optical OFDM (RPOOFDM) wasproposed to allow a higher degree of illumination control in theOFDMbased LiFi systems [44] RPOOFDM combines a realvalued optical OFDM broadband technique with slow PWM toallow dimming The dynamic range of the LED is fully used inRPOOFDM to minimize any nonlinear distortion The RPOOFDM is reported to achieve higher performance gains compared with DCOOFDM at a large fraction of dimming rangeswithout limiting the data rate of the system RPOOFDM offersa practical solution for the illumination and dimming controlfor LiFi communication systems however the OFDM signal inRPOOFDM is based on unipolar OFDM This means that theSE of RPOOFDM is half of that of DCOOFDM As a resultthe power efficiency advantage over DCOOFDM starts to diminish as the SE increases In addition the PWM duty cycle isassumed to be known at the receiver which means that sideinformation should be sent before any transmission and this requires perfect synchronization between the transmitting and receiving ends A novel technique that combines ACOOFDM onthe odd subcarriers with DCOOFDM on the even subcarrierswas proposed in asymmetrically DC biased optical OFDM(ADOOFDM) [45] The clipping noise of the ACOOFDM fallsonly into the even subcarriers and can be estimated and canceled with a 3 dB penalty at the receiver The power allocationfor different constellation sizes between ACOOFDM and DCOOFDM streams in ADOOFDM was investigated in [15] Theoptical power efficiency of the optimal settings for ADO OFDM was better than ACOOFDM and DCOOFDM for different configurations Hybrid asymmetrical clipped OFDM (HACOOFDM) uses ACOOFDM on the odd subcarriers and PAMDMT on the even subcarriers to improve the SE of unipolarOFDM modulation techniques [46] The asymmetrical clipping

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 6 (a) Bipolar OFDM waveform (b) UOFDM waveform

0 5 10

5

0

X U[n]

n(b)

0 5

X Bip[n]

5

-5

0 n

(a)Discrete time samples (s) Discrete time samples (s)

+ -

6

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

of the ACOOFDM on the odd symbols would only distort theeven subcarriers At the receiver ACOOFDM symbols are demodulated first by only considering the odd subcarriers andthen remodulated to estimate the ACOOFDM distortion on theeven subcarriers This allows the PAMDMT symbols on theeven subcarrier to be demodulated without any distortion TheSE achieved in HACO OFDM is identical to that of DCO OFDM however PAMDMT uses M PAM modulation on halfof the subcarriers Equal power was allocated to ACOOFDMand PAMDMT As the performance of M2QAM is equivalentto the performance of MPAM the power requirements for bothACOOFDM and PAMDMT to achieve the same performanceis different The problem also appears when different modulation orders are used for both schemes Unequal power allocation for both schemes was investigated in [47] to guarantee thatthe performance of both schemes in HACO OFDM is equalAn improved but computationally complex receiver was alsoproposed in [47] based on the time domain symmetry of bothACOOFDM and PAMDMT

Polar OFDM (POFDM) is a new method to achieve the IMDD for OFDM [48] The main principle of POFDM is to convert the complex valued output of the IFFT from the Cartesiancoordinates into the polar coordinates Therefore the radialand angular coordinate can be sent in the first and secondhalves of the OFDM frame successively It avoids the use ofHermitian symmetry however it allocates the M QAM symbols into the even indexed subcarriers As a result P OFDMhas halfwave even symmetry which states that the first half ofthe complex valued timedomain frame is identical to the otherhalf Therefore it is sufficient to transmit the first half of theIFFT output As a result the SE is reduced to be identical tothat of DCOOFDM since only half of the subcarriers are usedThe performance of P OFDM was compared to that of ACOOFDM in [49] It was reported that P OFDM achieves betterBER performance gains than ACO OFDM under narrow dynamic ranges when optimal values for the power allocation ofthe radial and angular information are used Note that any ISIbetween the radial and angular samples may deteriorate thesystem performance therefore the system performance in frequency selective channels should be investigated Asymmetrical and symmetrical clipping optical OFDM (ASCO OFDM)was proposed in [50] for IMDD Li Fi systems The ACO OFDM is combined with symmetrical clipping optical OFDM(SCOOFDM) that uses the even subcarriers The clipping distortion of both ACOOFDM and SCOOFDM affects the evensubcarriers However the clipping distortion of ACO OFDMcan be estimated and canceled at the receiver The SCO OFDM clipping noise can be removed at the receiver using UOFDMFlip OFDM time domain processing techniques TheSE of ASCOOFDM is 75 of the SE of DCOOFDM ASCOOFDM was reported to have better symbol error rate (SER)compared with ADOOFDM since the ADOOFDM uses theDC bias for the even subcarriers FIR filtering technique

termed spectral factorization was used to create a unipolar optical OFDM signal [51] The amplitude of the subcarriers inspectral factorized optical OFDM (SFOOFDM) were chosen toform an autocorrelation sequence that was shown to be sufficient to guarantee a unipolar OFDM output The SFOOFDMwas reported to achieve 05 dB gain over ACO OFDM with30 PAPR reduction [51] The position modulation OFDM(PMOFDM) avoids the Hermitian symmetry and splits the realand imaginary components of the OFDM output into twobranches where a polarity separator is used to obtain the positive and negative samples of each branch [52] The four framescomposed of a real positive frame a real negative one an imaginary positive one and an imaginary negative one are transmitted as unipolar OFDM frames The SE is exactly similar to other inherent unipolar OFDM techniques discussed in section41 The performance of PMOFDM was reported to be identical to UOFDM in flat channels However it was reported tohave better BER performance when compared to ACOOFDMfor frequency selective channels [52]43 Superposition OFDM Techniques

Superposition OFDM based modulation techniques rely onthe fact that the SE of UOFDMFlipOFDM ACOOFDM andPAMDMT can be doubled by proper superimposing of multiple layers of OFDM waveforms Superposition modulation wasfirst introduced for OFDM based OWC and has led to enhanced UOFDM (eUOFDM) [53] The eUOFDM compensates for the spectral efficiency loss of UOFDM by superimposing multiple UOFDM streams so that the interstreaminterference is null The generation method of the first depth ineUOFDM is exactly similar to that in UOFDM Subsequentdepths can be generated by UOFDM modulators before eachunipolar OFDM frame is repeated 2d1 times and scaled by 12d1where d is the depth number At the receiver the informationconveyed in the first depth is demodulated and then remodulated to be subtracted from the overall received signal Then repeated frames which are equivalent at higher depths are recombined and the demodulation procedure continues the same asfor the stream at the first depth Afterwards the informationconveyed in latter depths is demodulated in a similar way TheSE gap between UOFDM and DCOOFDM can never be completely closed with eU OFDM as this would require a largenumber of information streams to be superimposed in the modulation signal Implementation issues such as latency computational complexity power penalty and memory requirementsput a practical limit on the maximum number of availabledepths The eUOFDM was generalized in the Generalized Enhanced Unipolar OFDM (GREENER OFDM) for configurations where arbitrary constellation sizes and arbitrary power allocations are used [54] As a result the SE gap between U OFDM and DCOOFDM can be closed completely with an appropriate selection of the constellation sizes in different information streams The symmetry in UOFDM lies in frames

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 35

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

7

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

whilst in ACOOFDM and PAMDMT it lies in subframesThe superposition concept has also been extended to other

unipolar OFDM techniques such as PAMDMT [55] and ACOOFDM [56]- [60] The enhanced asymmetrically clipped optical OFDM (eACO OFDM) [56] uses the symmetry of ACO OFDM subframes to allow multiple ACOOFDM streams to besuperimposed A similar concept was also proposed by Elgalaet al and Wang et al under the names of spectrally and energyefficient OFDM (SEEOFDM) [57] and layered asymmetricallyclipped optical OFDM (Layered ACOOFDM) [58] respectively The receiver proposed in SEEOFDM [57] results in SNRpenalty that could have been avoided by using the symmetryproperties of ACOOFDM streams The symmetry arrangementin Layered ACOOFDM [58] is described in the frequency domain however it is shown in [58 Fig2] that it takes place inthe time domain Recently an alternative method to achievesuperposition modulation based on ACOOFDM was proposedby Kozu et al [59] for two ACOOFDM streams and Lawery[60] for Layered ACO OFDM This is similar in principle tothe solutions in [56]- [58] however the superposition is performed in the frequency domain which results in simpler system design The concept of eACO OFDM was generalized toclose the SE gap between ACOOFDM and DCOOFDM Thegeneration of eACOOFDM signal starts at the first depth withan ACOOFDM modulator Additional depths are generated ina similar way to the first depth but with an OFDM framelength equal to half of the previous depth frames Similar to eUOFDM all of the generated frames are repeated 2dminus1 times andappropriately scaled The demodulation process at the receiveris applied in a similar way as the eUOFDM The informationat Depth1 can be recovered directly as in conventional ACOOFDM because all of the inter stream interference falls intothe evenindexed subcarriers After the first stream is decodedthe information can be remodulated again and subtracted fromthe overall received signal Then the frames that are equivalent can be recombined and the demodulation procedure continues as for the stream at first depth

The enhanced pulse amplitude modulated discrete multi tone (ePAMDMT) [55] demonstrates that superposition modulation can also be utilized when the antisymmetry of PAM DMT waveforms is used Analogous to eUOFDM and eACOOFDM unique timedomain structures are also present in PAMDMT If the interference over a single PAMDMT frame possesses a Hermitian symmetry in the timedomain its frequencyprofile falls on the real component of the subcarriers Hencethe interference is completely orthogonal to the useful information which is encoded in imaginary symbols of the PAMDMTframes The concept of superposition modulation was extendedto ePAMDMT for an arbitrary modulation order and an arbitrary power allocation at each depth [55] The theoretical BERanalysis of eACOOFDM is similar to the analysis of GREENEROFDM therefore the optimal modulation sizes and scalingfactors are identical This is an expected result because the

performance of their unipolar OFDM forms ACOOFDM and UOFDM is also similar The ePAMDMT is less energy efficientthan GREENER OFDM and eACO OFDM because ePAMDMT has 3 dB loss in each depth demodulation process andthe optimal configurations of ePAM DMT are suboptimal asthe non squared M QAM BER performance can never beachieved using the M PAM modulation scheme The ePAMDMT is more energy efficient than DCOOFDM in terms of theelectrical SNR at SE values above 1 bitsHz In terms of theoptical SNR the ePAMDMT is less energy efficient than DCOOFDM for all of the presented values Higher optical energydissipation is a desirable property for illumination based LiFiapplications but it is considered as a disadvantage for dimmablebased LiFi applications However GREENEROFDM andeACOOFDM are suitable candidates for dimmablebased LiFi applications due to their optical SNR performance

5 Other MultiCarrier ModulationTechniquesOFDM has been mainly studied in the context of LiFi chan

nels based on FFT Other transformations such as discreteHartley transformation (DHT) [61] wavelet packet divisionmultiplexing (WPDM) [62] and Hadamard coded modulation(HCM) [63] have also been considered for Li Fi channels Amulticarrier IMDD system based on DHT was proposed in[61] It was shown that DHT output can be real when an inputframe of real modulated symbols such as binary phase shiftkeying (BPSK) and M PAM is used Similar to DCOOFDMand ACOOFDM DCbiasing and asymmetrical clipping canalso be used to achieve unipolar output in DHTbased multicarrier modulation technique As a major advantage over FFTbased conventional OFDM the DHTbased multicarrier modulation does not require any Hermitian symmetry However thisfails to improve the SE as real modulated symbols such as MPAM are used in DHTbased multicarrier modulation WPDMuses orthogonal wavelet packet functions for symbol modulation where the basis functions are wavelet packet functionswith finite length It was reported that the performance of WPDM is better than that of OFDM in terms of the spectral andpower efficiencies when LED nonlinear distortion and channeldispersion are taken into account [62] The high illuminationlevel of OFDM Li Fi systems require higher optical powerwhich may result in clipping due to the peak power constraintof the VL transfer function of the LED (Fig 2) HCM was proposed for multicarrier modulation LiFi as a solution to the limitation of OFDM modulation at higher illumination levels Thetechnique is based on fast Walsh Hadamard transformation(FWHT) as an alternative to the FFT HCM is reported toachieve higher performance gains when compared with ACOOFDM and DCO OFDM at higher illumination levels [63]However the performance improvement over RPO OFDM ismodest An alternative variant of HCM termed DC reduced

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS36

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

8

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 7: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

of the ACOOFDM on the odd symbols would only distort theeven subcarriers At the receiver ACOOFDM symbols are demodulated first by only considering the odd subcarriers andthen remodulated to estimate the ACOOFDM distortion on theeven subcarriers This allows the PAMDMT symbols on theeven subcarrier to be demodulated without any distortion TheSE achieved in HACO OFDM is identical to that of DCO OFDM however PAMDMT uses M PAM modulation on halfof the subcarriers Equal power was allocated to ACOOFDMand PAMDMT As the performance of M2QAM is equivalentto the performance of MPAM the power requirements for bothACOOFDM and PAMDMT to achieve the same performanceis different The problem also appears when different modulation orders are used for both schemes Unequal power allocation for both schemes was investigated in [47] to guarantee thatthe performance of both schemes in HACO OFDM is equalAn improved but computationally complex receiver was alsoproposed in [47] based on the time domain symmetry of bothACOOFDM and PAMDMT

Polar OFDM (POFDM) is a new method to achieve the IMDD for OFDM [48] The main principle of POFDM is to convert the complex valued output of the IFFT from the Cartesiancoordinates into the polar coordinates Therefore the radialand angular coordinate can be sent in the first and secondhalves of the OFDM frame successively It avoids the use ofHermitian symmetry however it allocates the M QAM symbols into the even indexed subcarriers As a result P OFDMhas halfwave even symmetry which states that the first half ofthe complex valued timedomain frame is identical to the otherhalf Therefore it is sufficient to transmit the first half of theIFFT output As a result the SE is reduced to be identical tothat of DCOOFDM since only half of the subcarriers are usedThe performance of P OFDM was compared to that of ACOOFDM in [49] It was reported that P OFDM achieves betterBER performance gains than ACO OFDM under narrow dynamic ranges when optimal values for the power allocation ofthe radial and angular information are used Note that any ISIbetween the radial and angular samples may deteriorate thesystem performance therefore the system performance in frequency selective channels should be investigated Asymmetrical and symmetrical clipping optical OFDM (ASCO OFDM)was proposed in [50] for IMDD Li Fi systems The ACO OFDM is combined with symmetrical clipping optical OFDM(SCOOFDM) that uses the even subcarriers The clipping distortion of both ACOOFDM and SCOOFDM affects the evensubcarriers However the clipping distortion of ACO OFDMcan be estimated and canceled at the receiver The SCO OFDM clipping noise can be removed at the receiver using UOFDMFlip OFDM time domain processing techniques TheSE of ASCOOFDM is 75 of the SE of DCOOFDM ASCOOFDM was reported to have better symbol error rate (SER)compared with ADOOFDM since the ADOOFDM uses theDC bias for the even subcarriers FIR filtering technique

termed spectral factorization was used to create a unipolar optical OFDM signal [51] The amplitude of the subcarriers inspectral factorized optical OFDM (SFOOFDM) were chosen toform an autocorrelation sequence that was shown to be sufficient to guarantee a unipolar OFDM output The SFOOFDMwas reported to achieve 05 dB gain over ACO OFDM with30 PAPR reduction [51] The position modulation OFDM(PMOFDM) avoids the Hermitian symmetry and splits the realand imaginary components of the OFDM output into twobranches where a polarity separator is used to obtain the positive and negative samples of each branch [52] The four framescomposed of a real positive frame a real negative one an imaginary positive one and an imaginary negative one are transmitted as unipolar OFDM frames The SE is exactly similar to other inherent unipolar OFDM techniques discussed in section41 The performance of PMOFDM was reported to be identical to UOFDM in flat channels However it was reported tohave better BER performance when compared to ACOOFDMfor frequency selective channels [52]43 Superposition OFDM Techniques

Superposition OFDM based modulation techniques rely onthe fact that the SE of UOFDMFlipOFDM ACOOFDM andPAMDMT can be doubled by proper superimposing of multiple layers of OFDM waveforms Superposition modulation wasfirst introduced for OFDM based OWC and has led to enhanced UOFDM (eUOFDM) [53] The eUOFDM compensates for the spectral efficiency loss of UOFDM by superimposing multiple UOFDM streams so that the interstreaminterference is null The generation method of the first depth ineUOFDM is exactly similar to that in UOFDM Subsequentdepths can be generated by UOFDM modulators before eachunipolar OFDM frame is repeated 2d1 times and scaled by 12d1where d is the depth number At the receiver the informationconveyed in the first depth is demodulated and then remodulated to be subtracted from the overall received signal Then repeated frames which are equivalent at higher depths are recombined and the demodulation procedure continues the same asfor the stream at the first depth Afterwards the informationconveyed in latter depths is demodulated in a similar way TheSE gap between UOFDM and DCOOFDM can never be completely closed with eU OFDM as this would require a largenumber of information streams to be superimposed in the modulation signal Implementation issues such as latency computational complexity power penalty and memory requirementsput a practical limit on the maximum number of availabledepths The eUOFDM was generalized in the Generalized Enhanced Unipolar OFDM (GREENER OFDM) for configurations where arbitrary constellation sizes and arbitrary power allocations are used [54] As a result the SE gap between U OFDM and DCOOFDM can be closed completely with an appropriate selection of the constellation sizes in different information streams The symmetry in UOFDM lies in frames

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 35

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

7

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

whilst in ACOOFDM and PAMDMT it lies in subframesThe superposition concept has also been extended to other

unipolar OFDM techniques such as PAMDMT [55] and ACOOFDM [56]- [60] The enhanced asymmetrically clipped optical OFDM (eACO OFDM) [56] uses the symmetry of ACO OFDM subframes to allow multiple ACOOFDM streams to besuperimposed A similar concept was also proposed by Elgalaet al and Wang et al under the names of spectrally and energyefficient OFDM (SEEOFDM) [57] and layered asymmetricallyclipped optical OFDM (Layered ACOOFDM) [58] respectively The receiver proposed in SEEOFDM [57] results in SNRpenalty that could have been avoided by using the symmetryproperties of ACOOFDM streams The symmetry arrangementin Layered ACOOFDM [58] is described in the frequency domain however it is shown in [58 Fig2] that it takes place inthe time domain Recently an alternative method to achievesuperposition modulation based on ACOOFDM was proposedby Kozu et al [59] for two ACOOFDM streams and Lawery[60] for Layered ACO OFDM This is similar in principle tothe solutions in [56]- [58] however the superposition is performed in the frequency domain which results in simpler system design The concept of eACO OFDM was generalized toclose the SE gap between ACOOFDM and DCOOFDM Thegeneration of eACOOFDM signal starts at the first depth withan ACOOFDM modulator Additional depths are generated ina similar way to the first depth but with an OFDM framelength equal to half of the previous depth frames Similar to eUOFDM all of the generated frames are repeated 2dminus1 times andappropriately scaled The demodulation process at the receiveris applied in a similar way as the eUOFDM The informationat Depth1 can be recovered directly as in conventional ACOOFDM because all of the inter stream interference falls intothe evenindexed subcarriers After the first stream is decodedthe information can be remodulated again and subtracted fromthe overall received signal Then the frames that are equivalent can be recombined and the demodulation procedure continues as for the stream at first depth

The enhanced pulse amplitude modulated discrete multi tone (ePAMDMT) [55] demonstrates that superposition modulation can also be utilized when the antisymmetry of PAM DMT waveforms is used Analogous to eUOFDM and eACOOFDM unique timedomain structures are also present in PAMDMT If the interference over a single PAMDMT frame possesses a Hermitian symmetry in the timedomain its frequencyprofile falls on the real component of the subcarriers Hencethe interference is completely orthogonal to the useful information which is encoded in imaginary symbols of the PAMDMTframes The concept of superposition modulation was extendedto ePAMDMT for an arbitrary modulation order and an arbitrary power allocation at each depth [55] The theoretical BERanalysis of eACOOFDM is similar to the analysis of GREENEROFDM therefore the optimal modulation sizes and scalingfactors are identical This is an expected result because the

performance of their unipolar OFDM forms ACOOFDM and UOFDM is also similar The ePAMDMT is less energy efficientthan GREENER OFDM and eACO OFDM because ePAMDMT has 3 dB loss in each depth demodulation process andthe optimal configurations of ePAM DMT are suboptimal asthe non squared M QAM BER performance can never beachieved using the M PAM modulation scheme The ePAMDMT is more energy efficient than DCOOFDM in terms of theelectrical SNR at SE values above 1 bitsHz In terms of theoptical SNR the ePAMDMT is less energy efficient than DCOOFDM for all of the presented values Higher optical energydissipation is a desirable property for illumination based LiFiapplications but it is considered as a disadvantage for dimmablebased LiFi applications However GREENEROFDM andeACOOFDM are suitable candidates for dimmablebased LiFi applications due to their optical SNR performance

5 Other MultiCarrier ModulationTechniquesOFDM has been mainly studied in the context of LiFi chan

nels based on FFT Other transformations such as discreteHartley transformation (DHT) [61] wavelet packet divisionmultiplexing (WPDM) [62] and Hadamard coded modulation(HCM) [63] have also been considered for Li Fi channels Amulticarrier IMDD system based on DHT was proposed in[61] It was shown that DHT output can be real when an inputframe of real modulated symbols such as binary phase shiftkeying (BPSK) and M PAM is used Similar to DCOOFDMand ACOOFDM DCbiasing and asymmetrical clipping canalso be used to achieve unipolar output in DHTbased multicarrier modulation technique As a major advantage over FFTbased conventional OFDM the DHTbased multicarrier modulation does not require any Hermitian symmetry However thisfails to improve the SE as real modulated symbols such as MPAM are used in DHTbased multicarrier modulation WPDMuses orthogonal wavelet packet functions for symbol modulation where the basis functions are wavelet packet functionswith finite length It was reported that the performance of WPDM is better than that of OFDM in terms of the spectral andpower efficiencies when LED nonlinear distortion and channeldispersion are taken into account [62] The high illuminationlevel of OFDM Li Fi systems require higher optical powerwhich may result in clipping due to the peak power constraintof the VL transfer function of the LED (Fig 2) HCM was proposed for multicarrier modulation LiFi as a solution to the limitation of OFDM modulation at higher illumination levels Thetechnique is based on fast Walsh Hadamard transformation(FWHT) as an alternative to the FFT HCM is reported toachieve higher performance gains when compared with ACOOFDM and DCO OFDM at higher illumination levels [63]However the performance improvement over RPO OFDM ismodest An alternative variant of HCM termed DC reduced

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS36

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

8

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 8: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

whilst in ACOOFDM and PAMDMT it lies in subframesThe superposition concept has also been extended to other

unipolar OFDM techniques such as PAMDMT [55] and ACOOFDM [56]- [60] The enhanced asymmetrically clipped optical OFDM (eACO OFDM) [56] uses the symmetry of ACO OFDM subframes to allow multiple ACOOFDM streams to besuperimposed A similar concept was also proposed by Elgalaet al and Wang et al under the names of spectrally and energyefficient OFDM (SEEOFDM) [57] and layered asymmetricallyclipped optical OFDM (Layered ACOOFDM) [58] respectively The receiver proposed in SEEOFDM [57] results in SNRpenalty that could have been avoided by using the symmetryproperties of ACOOFDM streams The symmetry arrangementin Layered ACOOFDM [58] is described in the frequency domain however it is shown in [58 Fig2] that it takes place inthe time domain Recently an alternative method to achievesuperposition modulation based on ACOOFDM was proposedby Kozu et al [59] for two ACOOFDM streams and Lawery[60] for Layered ACO OFDM This is similar in principle tothe solutions in [56]- [58] however the superposition is performed in the frequency domain which results in simpler system design The concept of eACO OFDM was generalized toclose the SE gap between ACOOFDM and DCOOFDM Thegeneration of eACOOFDM signal starts at the first depth withan ACOOFDM modulator Additional depths are generated ina similar way to the first depth but with an OFDM framelength equal to half of the previous depth frames Similar to eUOFDM all of the generated frames are repeated 2dminus1 times andappropriately scaled The demodulation process at the receiveris applied in a similar way as the eUOFDM The informationat Depth1 can be recovered directly as in conventional ACOOFDM because all of the inter stream interference falls intothe evenindexed subcarriers After the first stream is decodedthe information can be remodulated again and subtracted fromthe overall received signal Then the frames that are equivalent can be recombined and the demodulation procedure continues as for the stream at first depth

The enhanced pulse amplitude modulated discrete multi tone (ePAMDMT) [55] demonstrates that superposition modulation can also be utilized when the antisymmetry of PAM DMT waveforms is used Analogous to eUOFDM and eACOOFDM unique timedomain structures are also present in PAMDMT If the interference over a single PAMDMT frame possesses a Hermitian symmetry in the timedomain its frequencyprofile falls on the real component of the subcarriers Hencethe interference is completely orthogonal to the useful information which is encoded in imaginary symbols of the PAMDMTframes The concept of superposition modulation was extendedto ePAMDMT for an arbitrary modulation order and an arbitrary power allocation at each depth [55] The theoretical BERanalysis of eACOOFDM is similar to the analysis of GREENEROFDM therefore the optimal modulation sizes and scalingfactors are identical This is an expected result because the

performance of their unipolar OFDM forms ACOOFDM and UOFDM is also similar The ePAMDMT is less energy efficientthan GREENER OFDM and eACO OFDM because ePAMDMT has 3 dB loss in each depth demodulation process andthe optimal configurations of ePAM DMT are suboptimal asthe non squared M QAM BER performance can never beachieved using the M PAM modulation scheme The ePAMDMT is more energy efficient than DCOOFDM in terms of theelectrical SNR at SE values above 1 bitsHz In terms of theoptical SNR the ePAMDMT is less energy efficient than DCOOFDM for all of the presented values Higher optical energydissipation is a desirable property for illumination based LiFiapplications but it is considered as a disadvantage for dimmablebased LiFi applications However GREENEROFDM andeACOOFDM are suitable candidates for dimmablebased LiFi applications due to their optical SNR performance

5 Other MultiCarrier ModulationTechniquesOFDM has been mainly studied in the context of LiFi chan

nels based on FFT Other transformations such as discreteHartley transformation (DHT) [61] wavelet packet divisionmultiplexing (WPDM) [62] and Hadamard coded modulation(HCM) [63] have also been considered for Li Fi channels Amulticarrier IMDD system based on DHT was proposed in[61] It was shown that DHT output can be real when an inputframe of real modulated symbols such as binary phase shiftkeying (BPSK) and M PAM is used Similar to DCOOFDMand ACOOFDM DCbiasing and asymmetrical clipping canalso be used to achieve unipolar output in DHTbased multicarrier modulation technique As a major advantage over FFTbased conventional OFDM the DHTbased multicarrier modulation does not require any Hermitian symmetry However thisfails to improve the SE as real modulated symbols such as MPAM are used in DHTbased multicarrier modulation WPDMuses orthogonal wavelet packet functions for symbol modulation where the basis functions are wavelet packet functionswith finite length It was reported that the performance of WPDM is better than that of OFDM in terms of the spectral andpower efficiencies when LED nonlinear distortion and channeldispersion are taken into account [62] The high illuminationlevel of OFDM Li Fi systems require higher optical powerwhich may result in clipping due to the peak power constraintof the VL transfer function of the LED (Fig 2) HCM was proposed for multicarrier modulation LiFi as a solution to the limitation of OFDM modulation at higher illumination levels Thetechnique is based on fast Walsh Hadamard transformation(FWHT) as an alternative to the FFT HCM is reported toachieve higher performance gains when compared with ACOOFDM and DCO OFDM at higher illumination levels [63]However the performance improvement over RPO OFDM ismodest An alternative variant of HCM termed DC reduced

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS36

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

8

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 9: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

HCM (DCRHCM) was also proposed to reduce the power consumption of HCM to support dimmable LiFi applications andinterleaving with MMSE equalization is used for HCM in dispersive LiFi channels

6 LiFi Unique Modulation TechniqueThe modulation frequency in LiFi systems does not corre

spond to the carrier frequency of the LED All the aforementioned modulation techniques are baseband modulation techniques It is practically difficult to modulate the carrier frequency of the LEDs however it is practically straightforwardto change its colour This feature adds a new degree of freedomto Li Fi systems Colour tunable LEDs such as the red greenblue LED (RGB LED) can illuminate with different coloursbased on the intensity applied on each LED element TheIEEE 802157 standard proposes colour shift keying (CSK) asa modulation technique for VLC [8] The incoming bits aremapped into a constellation of colours from the chromatic CIE1931 colour space [64] as shown in Fig 7 The CIE 1931 isthe widely used illumination model for human eye colour perception Any colour in the model can be represented by thechromaticity dimension [x y] In CSK the overall intensity ofthe output colour is constant however the relative intensitiesbetween the multiple used colours are changed Therefore theinstantaneous colour of the multicolour LED is modulated Seven wavelengths are defined in IEEE 802157 specify the vertices of a triangle where the constellation point lies in The intensity of each RGBLED element is changed to match the constellation point while maintaining a constant optical power anda constant illumination colour This is desirable in Li Fi systems since the constant illumination colour naturally mitigatesany flickering An amplitude dimming is used for brightnesscontrol in CSK while the center colour of the colour constella

tion constant is kept However colour shift is possible due tothe presence of any improper driving current used for dimmingcontrol Constellation sizes up to 16CSK were proposed in theIEEE 802157 standard based on tricolour LEDs Constellation points design based on CIE 1931 was also investigated byDrost and Sadler using billiard algorithms [65] by Monterioand Hranilovic using interior point method [66] by Singh et alusing quad LED (QLED) [67] and by Jiang et al using extrinsic transfer (EXIT) charts for an iterative CSK transceiver design [68]

A generalized CSK (GCSK) that operates under varying target colours independent from the number of used LEDs wasproposed in [69] Colour intensity modulation (CIM) was proposed to improve the communication capacity without any lossto the illumination properties (dimming and target colourmatching) [70] The instantaneous intensity of the RGB LEDwas modulated in CIM while only maintaining a constant perceived colour Therefore CIM can be considered as a relaxedversion of CSK since a constant perceived power is additionally required in CSK Metameric modulation (MM) constrains theCSK to have a constant instantaneous perceived ambient lightwith the aid of an external green LED [70] An improved control of the RGB output colour was achieved in MM by improving the colour rendering and reducing the colour flickering[71] A four colour system was used in [67] with the aid of additional IMDD signaling as a fourth dimension signal Higher order modulation techniques of 212CSK for QLED were achievedin [67]The CSK was combined with constant rate differentialPPM in [72] to simplify the synchronization while maintainingthe illumination control and avoiding flickering A similar approach of combining CSK with complementary PPM was proposed by [73] A digital CSK (DCSK) was proposed in [74]Multiple multicolour LEDs were used in DCSK where only onecolour is activated in each multicolour LED at a single timeTherefore the information is encoded in the combinations of activated colours The main advantage of DCSK over conventional CSK is avoiding the need of any digitaltoanalog converterswhile the main disadvantage is rendering the activated colourswhich may result in slight changes of the colour perceptionover time

The receiver architecture has not been fully addressed inmost of the published research on colour domain modulationCSK is considered to be an expensive and complex modulationtechnique when compared with OFDM The colour dimensionin LiFi can also be used to derive a multicolour LED with different streams of data The optical summation may turn this coloured parallel stream into a single colour stream output thatcan be filtered at the receiver into the original transmitted coloured stream

7 ConclusionsThe modulation techniques suitable for LiFi are presented

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 37

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Figure 7 The symbol mapping of 4CSK on the CIE 1931 colourmodel based on IEEE 802157

0807060504030201

080604020x

y

(00)

(11)(01)

(10)

9

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 10: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

in this paper These techniques should satisfy illumination andcommunication requirements Single carrier modulation techniques offer a simple solution for frequency flat Li Fi channels Lowtomedium data rates can be achieved using singlecarrier modulation techniques Multicarrier modulation techniques offer high data rates solution that can adapt the systemperformance to the channel frequency response Many variantsof optical OFDM modulation techniques have been proposedin published research to satisfy certain illumination andorcommunication requirements A summary of LiFi multicarriermodulation techniques is presented in Table 1 The colour di

mension offers unique modulation formats for LiFi and adds tothe degrees of freedom of Li Fi systems Time frequencyspace colour dimensions and the combinations of them can beused for LiFi modulation LiFi modulation techniques shouldoffer a high speed communication and be suitable for most illumination regimesAcknowledgment

The authors would like to thank Tezcan Cogalan and LiangYin for their valuable comments and suggestions that improvedthe presentation of the paper

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS38

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

Table 1 Comparison of multicarrier modulation schemes for LiFi

Mod Tech

ADOOFDMDCOOFDMInherentunipolar

Spatial OFDMRPOOFDM

HACOOFDM

POFDMASCOOFDMSFOOFDMPMOFDM

Superposition

DHTWPDMHCM

SE as afunction ofDCOOFDM

100100

50

10050

100

5075

Variable50

100

50100100100

IlluminationControl

NoNo

No

LimitedYes

No

NoNoNoNo

No

NoNoYes

LevelDimmedmediumMedium

Dimmed

MediumDimmed

high

Dimmed

MediumDimmedMediumMedium

DimmedDimmedmediumMediumHigh

Computationalcomplexity

HighLow

Low

HighMedium

High

HighHighHighHigh

High

LowHighLow

RemarksRequiresDC biasRequiresDC biasPower

efficient atlow SE

Low PAPRRequires

syncPower

efficient atlowmedium

SE

Low PAPR

Powerefficient atlowhigh SE

Powerinefficient

Ref

[15][26]

[30]-[33]

[43][44]

[46]

[48][50][51][52]

[53]-[60]

[61][62][63]

References[1] Cisco (2016 Feb) Global mobile data traffic forecast update 20152020 [On

line] Available httpwwwciscocomcenussolutionscollateralserviceprovidervisualnetworkingindexvnimobilewhitepaperc11520862pdf

[2] S Dimitrov and H Haas Principles of LED Light Communications Towards Networked LiFi Cambridge England Cambridge University Press 2015

[3] D Tsonev S Videv and H HaasldquoTowards a 100 Gbs visible light wireless access networkrdquoOptics Express vol 23 no 2 pp 1627-1637 Jan 2015 doi101364OE23001627

[4] H Elgala R Mesleh and H HaasldquoA study of LED nonlinearity effects on optical wireless transmission using OFDMrdquoin Proc 6th IEEE International Conference on Wireless and Optical Communications Networks (WOCN) Cairo EgyptApr 28-30 2009 doi 101109WOCN20095010576

[5] A M Khalid G Cossu R Corsini et alldquo1Gbs transmission over a phosphorescent white LED by using rateadaptive discrete multitone modulationrdquoIEEEPhotonics Journal vol 4 no 5 pp 1465- 1473 Oct 2012 doi 101109JPHOT20122210397

[6] G Cossu A M Khalid P Choudhury et alldquo34 Gbits visible optical wirelesstransmission based on RGB LEDrdquoOptics Express vol 20 pp B501- B5062012 doi 101364OE2000B501

[7] J M Kahn and J R BarryldquoWireless infrared communicationsrdquoProceedings ofthe IEEE vol 85 no 2 pp 265-298 Feb 1997

[8] IEEE Standard for Local and Metropolitan Area Networks Part 157 Short Range Wireless Optical Communication Using Visible Light IEEE Std 8021572011 2011 doi 101109IEEESTD20116016195

[9] S Randel F Breyer S C J Lee et alldquoAdvanced modulation schemes forshortrange optical communicationsrdquoIEEE Journal of Selected Topics in Quantum Electronics vol PP no 99 pp 1 - 10 2010 doi 101109JSTQE20102040808

[10] D Shan Shiu and J KahnldquoDifferential pulseposition modulation for powerefficient optical communicationrdquoIEEE Transactions on Communications vol47 no 8 pp 1201-1210 Aug 1999 doi 10110926780456

[11] F Delgado I Quintana J Rufo et alldquoDesign and implementation of an Ethernet VLC interface for broadcast transmissionsrdquoIEEE Communications Letters vol 14 no 12 pp 1089- 1091 Dec 2010 doi 101109LCOMM201012100984

[12] S H Lee SY Jung and J K KwonldquoModulation and coding for dimmablevisible light communicationrdquoIEEE Communications Magazine vol 53 no 2pp 136-143 Feb 2015 doi 101109MCOM20157045402

[13] Y Zeng R Green and M LeesonldquoMultiple pulse amplitude and positionmodulation for the optical wireless channelrdquoin Proc 10th Anniversary International Conference on Transparent Optical Networks (ICTONrsquo08) vol 4 AthensGreece Jun 22-26 2008 pp 193-196 doi 101109ICTON20084598766

[14] R Mesleh H Elgala and H HaasldquoOn the performance of different OFDMbased optical wireless communication systemsrdquoIEEEOSA Journal of OpticalCommunications and Networking vol 3 no 8 pp 620-628 Aug 2011 doi101364JOCN3000620

[15] S Dissanayake and J ArmstrongldquoComparison of ACOOFDM DCOOFDMand ADO OFDM in IMDD systemsrdquoJournal of Lightwave Technology vol31 no 7 pp 1063-1072 Apr 2013 doi 101109JLT20132241731

[16] D Barros S Wilson and J KahnldquoComparison of orthogonal frequencydivision multiplexing and pulse amplitude modulation in indoor optical wirelesslinksrdquoIEEE Transactions on Communications vol 60 no 1 pp 153- 1632012 doi 101109TCOMM2011112311100538

[17] J Armstrong and B J C SchmidtldquoComparison of asymmetrically clipped optical OFDM and DCbiased optical OFDM in AWGNrdquoIEEE CommunicationsLetters vol 12 no 5 pp 343- 345 May 2008 doi 101109LCOMM2008080193

[18] M Kashani and M KavehradldquoOn the performance of single and multicarriemodulation schemes for indoor visible light communication systemsrdquoin IEEEGlobal Communications Conference (GLOBECOM) Austin USA Dec 2014pp 2084-2089 doi 101109GLOCOM20147037115

[19] J B Carruthers and J M KahnldquoAngle diversity for nondirected wireless infrared communicationrdquoIEEE Transactions on Communications vol 48 no 6pp 960-969 Jun 2000 doi 10110926848557

[20] J G Proakis Digital Communications 4th ed New York USA McGraw-Hill2000

[21] K Acolatse Y BarNess and S K WilsonldquoNovel techniques of singlecarrier frequencydomain equalization for optical wireless communicationsrdquoEURASIP Journal on Advances in Signal Processing vol 2011 pp 41-413 Jan2011 [Online] Available 1011552011393768

[22] C Chen Hsieh and D Shan ShiuldquoSingle carrier modulation with frequency domain equalization for intensity modulationdirect detection channels with intersymbol interferencerdquoin 17th IEEE International Symposium on Personal Indoor and Mobile Radio Communications Helsinki Finland Sept 2006 pp 1-5 doi 101109PIMRC2006254418

10

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 11: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2 ZTE COMMUNICATIONSZTE COMMUNICATIONS 39

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

[23] A Nuwanpriya J Zhang A Grant et alldquoSingle carrier frequency domainequalization based on onoff keying for optical wireless communicationsrdquoinIEEE Wireless Communications and Networking Conference (WCNC) ShanghaiChina Apr 2013 pp 4272-4277 doi 101109WCNC20136555264

[24] C Wu H Zhang and W XuldquoOn visible light communication using led arraywith DFT spread OFDMrdquoin IEEE International Conference on Communications (ICC) Sydney Australia Jun 2014 pp 3325- 3330 doi 101109ICC20146883834

[25] P Haigh S T Le S Zvanovec et alldquoMultiband carrierless amplitude andphase modulation for bandlimited visible light communications systemsrdquoIEEEWireless Communications vol 22 no 2 pp 46-53 Apr 2015 doi 101109MWC20157096284

[26] J B Carruthers and J M KahnldquoMultiplesubcarrier modulation for nondirected wireless infrared communicationrdquoIEEE Journal on Selected Areas in Communications vol 14 no 3 pp 538-546 Apr 1996 doi 10110949490239

[27] S Dimitrov and H HaasldquoInformation rate of OFDMbased optical wirelesscommunication systems with nonlinear distortionrdquoIEEE Journal of LightwaveTechnology vol 31 no 6 pp 918- 929 Mar 2013 doi 101109JLT20122236642

[28] X Ling J Wang X Liang et alldquoOffset and power optimization for DCOOFDM in visible light communication systemsrdquoIEEE Transactions on SignalProcessing vol 64 no 2 pp 349- 363 Jan 2016 doi 101109TSP20152477799

[29] M Zhang and Z ZhangldquoAn optimum DCbiasing for DCOOFDM systemrdquoIEEE Communications Letters vol 18 no 8 pp 1351-1354 Aug 2014 doi101109LCOMM20142331068

[30] J Armstrong and A LoweryldquoPower efficient optical OFDMrdquoElectronics Letters vol 42 no 6 pp 370-372 Mar 2006 doi 101049el20063636

[31] S C J Lee S Randel F Breyer et alldquoPAMDMT for intensitymodulatedand directdetection optical communication systemsrdquoIEEE Photonics Technology Letters vol 21 no 23 pp 1749- 1751 Dec 2009 doi 101109LPT20092032663

[32] N Fernando Y Hong and E ViterboldquoFlipOFDM for unipolar communication systemsrdquoIEEE Transactions on Communications vol 60 no 12 pp3726-3733 Dec 2012 doi 101109TCOMM2012082712110812

[33] D Tsonev S Sinanovic and H HaasldquoNovel unipolar orthogonal frequency division multiplexing (UOFDM) for optical wirelessrdquoin Proc IEEE VehicularTechnology Conference (VTC Spring) Yacuteokohama Japan May 2012 doi101109VETECS20126240060

[34] L Chen B Krongold and J EvansldquoDiversity combining for asymmetricallyclipped optical OFDM in IMDD channelsrdquoin IEEE Global Telecommunications Conference (GLOBECOM 2009) Hawaii USA Nov 2009 pp 1-6 doi101109GLOCOM20095425293

[35] J Dang Z Zhang and L WuldquoA novel receiver for ACOOFDM in visiblelight communicationrdquoIEEE Communications Letters vol 17 no 12 pp 2320-2323 Dec 2013 doi 101109LCOMM2013111113132223

[36] N Huang JB Wang C Pan et alldquoIterative receiver for flipOFDM in optical wireless communicationrdquoIEEE Photonics Technology Letters vol 27 no16 pp 1729-1732 Aug 2015 doi 101109LPT20152438338

[37] Y Zheng Z Zhang J Dang et alldquoA novel receiver for flipOFDM in opticalwireless communicationrdquoin IEEE 16th International Conference on Communication Technology (ICCT) Mumbai India Oct 2015 pp 620- 625 doi101109ICCT20157399914

[38] J Dang Z Zhang and L WuldquoFrequencydomain diversity combining receiver for ACOOFDM systemrdquoIEEE Photonics Journal vol 7 no 6 pp 1-10Dec 2015 doi 101109JPHOT20152496865

[39] J Xu W Xu H Zhang et alldquoAsymmetrically reconstructed optical OFDMfor visible light communicationsrdquoIEEE Photonics Journal vol 8 no 1 pp 1-18 Feb 2016 doi 101109JPHOT20162520818

[40] N Huang JB Wang J Wang et alldquoReceiver design for PAMDMT in indoor optical wireless linksrdquoIEEE Photonics Technology Letters vol 27 no 2pp 161-164 Jan 2015 doi 101109LPT20142363876

[41] N Xiang Z Zhang J Dang et alldquoA novel receiver design for PAMDMT inoptical wireless communication systemsrdquoIEEE Photonics Technology Lettersvol 27 no 18 pp 1919-1922 Sept 2015 doi 101109LPT20152445793

[42] L Wu Z Zhang J Dang et alldquoAdaptive modulation schemes for visiblelight communicationsrdquoJournal of Lightwave Technology vol 33 no 1 pp117-125 Jan 2015 doi 101109JLT20142374171

[43] M Mossaad S Hranilovic and L LampeldquoVisible light communications usingOFDM and multiple LEDsrdquoIEEE Transactions on Communications vol 63no 11 pp 4304-4313 Nov 2015 doi 101109TCOMM20152469285

[44] H Elgala and T D C LittleldquoReverse polarity opticalOFDM (RPOOFDM)

dimming compatible OFDM for gigabit VLC linksrdquoOptics Express vol 21 no20 pp 24288-24299 Oct 2013 doi 101364OE21024288

[45] S Dissanayake K Panta and J ArmstrongldquoA novel technique to simultaneously transmit ACO OFDM and DCO OFDM in IMDD systemsrdquoin IEEEGLOBECOM Workshops (GC Wkshps) Houston USA Dec 2011 pp 782-786doi 101109GLOCOMW20116162561

[46] B Ranjha and M KavehradldquoHybrid asymmetrically clipped OFDMbased IMDD optical wireless systemrdquoIEEEOSA Journal of Optical Communicationsand Networking vol 6 no 4 pp 387- 396 Apr 2014 doi 101364JOCN6000387

[47] Q Wang Z Wang and L DaildquoIterative receiver for hybrid asymmetricallyclipped optical OFDMrdquoJournal of Lightwave Technology vol 32 no 22 pp4471-4477 Nov 2014 doi 101109JLT20142358611

[48] H Elgala and T LittleldquoPOFDM Spectrally efficient unipolar OFDMrdquoin Optical Fiber Communications Conference and Exhibition (OFC) San FranciscoUSA Mar 2014 pp 1-3 doi101364OFC2014Th3G7

[49] H Elgala and T D C LittleldquoPolarbased OFDM and SCFDE links toward energyefficient GBPS transmission under IMDD optical system constraints invitedrdquoJournal of Optical Communications and Networking vol 7 no 2 ppA277-A284 Feb 2015 doi 101364JOCN700A277

[50] N Wu and Y BarNessldquoA novel powerefficient scheme asymmetrically andsymmetrically clipping optical (ASCO) OFDM for IMDD optical systemsrdquoEURASIP Journal on Advances in Signal Processing vol 2015 no 1 pp 1-10 2015 doi 1011861687618020153

[51] K Asadzadeh A Farid and S HranilovicldquoSpectrally factorized opticalOFDMrdquoin IEEE 12th Canadian Workshop on Information Theory (CWIT2011) British Columbia Canada May 2011 pp 102- 105 doi 101109CWIT20115872134

[52] T Mao C Qian Q Wang et alldquoPMDCOOFDM for PAPR reduction in visible light communicationsrdquoin Opto Electronics and Communications Conference (OECC) Shanghai China Jun 2015 pp 1- 3 doi 101109OECC20157340207

[53] D Tsonev and H HaasldquoAvoiding spectral efficiency loss in Unipolar OFDMfor optical wireless communicationrdquoin Proc International Conference on Communications (ICC) Sydney Australia Jun 2014 doi 101109ICC20146883836

[54] M Islim D Tsonev and H HaasldquoA generalized solution to the spectral efficiency loss in unipolar optical OFDMbased systemsrdquoin Proc IEEE International Conference on Communications (ICC) London UK Jun 2015 doi101109ICC20157249137

[55] M Islim D Tsonev and H HaasldquoSpectrally enhanced PAMDMT for IMDDoptical wireless communicationsrdquoin Proc IEEE 25th Int Symp Pers Indoorand Mobile Radio Commun (PIMRC) Hong Kong China 2015 pp 927-932doi 101109PIMRC20157343421

[56] M Islim D Tsonev and H HaasldquoOn the superposition modulation for OFDMbased optical wireless communicationrdquoin IEEE Global Conference on Signaland Information Processing (GlobalSIP) Orlando USA Dec 2015 doi101109GlobalSIP20157418352

[57] H Elgala and T LittleldquoSEEOFDM Spectral and energy efficient OFDM foroptical IMDD systemsrdquoin IEEE 25th Annual International Symposium on Personal Indoor and Mobile Radio Communication (PIMRC) Washington DCUSA 2014 pp 851-855 doi 101109PIMRC20147136284

[58] Q Wang C Qian X Guo et alldquoLayered ACOOFDM for intensitymodulated directdetection optical wireless transmissionrdquoOptics Express vol 23 no9 pp 12382-12393 May 2015 doi 101364OE23012382

[59] T Kozu and K OhuchildquoProposal for superposed ACOOFDM using severaleven subcarriersrdquoin 9th International Conference on Signal Processing andCommunication Systems (ICSPCS) Cairns Australia Dec 2015 pp 1-5 doi101109ICSPCS20157391762

[60] A J LoweryldquoComparisons of spectrallyenhanced asymmetricallyclipped optical OFDM systemsrdquoOptics Express vol 24 no 4 pp 3950-3966 2016 doi101364OE24003950

[61] M S Moreolo R M noz and G JunyentldquoNovel power efficient opticalOFDM based on Hartley transform for intensitymodulated directdetection systemsrdquoJournal of Lightwave Technology vol 28 no 5 pp 798- 805 Mar2010 doi 101109JLT20102040580

[62] W Huang C Gong and Z XuldquoSystem and waveform design for wavelet packet division multiplexingbased visible light communicationsrdquoJournal of Lightwave Technology vol 33 no 14 pp 3041- 3051 Jul 2015 doi 101109JLT20152418752

[63] M Noshad and M Brandt PearceldquoHadamard coded modulation for visiblelight communicationsrdquoIEEE Transactions on Communications vol PP no 99

11

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12

Page 12: ModulationTechniquesforLi⁃ · PDF fileLi⁃Fi:lightfidelity MCM:multicarriermodulation MM:metamericmodulation M⁃PAM:M⁃arypulseamplitudemodulation M⁃PPM:M⁃arypulsepositionmodulation

DEMAG2016-04-50VOL13F5VFTmdashmdash12PPSP

Special Topic

April 2016 Vol14 No2ZTE COMMUNICATIONSZTE COMMUNICATIONS40

Modulation Techniques for LiFiMohamed Sufyan Islim and Harald Haas

pp 1-1 2016 doi 101109TCOMM20162520471[64] The International Commission on Illumination (CIE) (2008 Aug) CIE 1931

standard colorimetric observer [Online] Available httpwwwciecoat[65] R Drost and B SadlerldquoConstellation design for colorshift keying using bil

liards algorithmsrdquoin IEEE GLOBECOM Workshops (GC Wkshps) MiamiUSA Dec 2010 pp 980-984 doi 101109GLOCOMW20105700472

[66] E Monteiro and S HranilovicldquoDesign and implementation of colorshift keying for visible light communicationsrdquoJournal of Lightwave Technology vol32 no 10 pp 2053-2060 May 2014 doi 101109JLT20142314358

[67] R Singh T OrsquoFarrell and J P R DavidldquoAn enhanced color shift keyingmodulation scheme for high speed wireless visible light communicationsrdquoJournal of Lightwave Technology vol 32 no 14 pp 2582-2592 Jul 2014doi 101109JLT20142328866

[68] J Jiang R Zhang and L HanzoldquoAnalysis and design of threestage concatenated colorshift keyingrdquoIEEE Transactions on Vehicular Technology vol 64no 11 pp 5126-5136 Nov 2015 doi 101109TVT20142382875

[69] N Murata H Shimamoto Y Kozawa et alldquoPerformance evaluation of digitalcolour shift keying for visible light communicationsrdquoin IEEE InternationalConference on Communication Workshop (ICCW) London UK Jun 2015 pp1374-1379 doi 101109ICCW20157247370

[70] K I Ahn and J KwonldquoColor intensity modulation for multicolored visiblelight communicationsrdquoIEEE Photonics Technology Letters vol 24 no 24 pp2254-2257 Dec 2012 doi 101109LPT20122226570

[71] P Butala J Chau and T LittleldquoMetameric modulation for diffuse visiblelight communications with constant ambient lightingrdquoin International Workshop on Optical Wireless Communications (IWOW) Pisa Italy Oct 2012 pp1-3 doi 101109IWOW20126349697

[72] J LunaRivera R PerezJimenez V GuerraYantildeez et alldquoCombined CSKand pulse position modulation scheme for indoor visible light communicationsrdquoElectronics Letters vol 50 no 10 pp 762- 764 May 2014 doi101049el20140953

[73] S Pergoloni M Biagi S Colonnese et alldquoMerging color shift keying andcomplementary pulse position modulation for visible light illumination andcommunicationrdquoin Euro Med Telco Conference (EMTC) Naples Italy Nov2014 pp 1-6 doi 101109EMTC20146996621

[74] F Delgado RajoIgrave V Guerra J RabadaIgraven Borges et alldquoColor shift keyingcommunication system with a modified PPM synchronization schemerdquoIEEE

on Photonics Technology Letters vol 26 no 18 pp 1851-1854 Sept 2014doi 101109LPT20142337953

Manuscript received 20160224

Mohamed Sufyan Islim (mislimedacuk) received his BSc (1st Hons) in communications technology engineering in 2009 and MSc (Distinction) in communicationsengineering from Aleppo University Syria in 2012 Among several scholarships hewas awarded in 2013 he was awarded the Global Edinburgh Scholarship from Edinburgh University UK In 2014 he received another MSc (Distinction) in signal processing and communications from Edinburgh University He was the recipient of the2014 IEEE Communications Chapter Best Master Project Prize Currently he is aPhD student under the supervision of Professor Harald Haas at the LiFi Researchand Development Centre University of Edinburgh His research interests includeoptical OFDM LiFi and optical wireless communicationsHarald Haas (hhaasedacuk) holds the chair for Mobile Communications at theSchool of Engineering and is the director of the LiFi Research and DevelopmentCentre University of Edinburgh UK Professor Haas has been working in wirelesscommunications for 20 years and has held several posts in industry He was an invited speaker at TED Global in 2011 where he demonstrated and coinedldquoLiFirdquo LiFiwas listed among the 50 best inventions in TIME Magazine 2011 Moreover hiswork has been covered in other international media such as the New York TimesBBC MSNBC CNN International Wired UK and many more He is initiator cofounder and chief scientific officer (CSO) of pureLiFi Ltd Professor Haas holds 31patents and has more than 30 pending patent applications He has published 300conference and journal papers including a paper in Science Magazine He publishedtwo textbooks with Cambridge University Press His hindex is 43 (Google) In 2015he was corecipient of three best paper awards including the IEEE Jack NeubauerMemorial Award He is CI of programme grant TOUCAN (EPL0200091) and CI ofSERAN (EPL0261471) He currently holds an EPSRC Established Career Fellowship (EPK0087571) In 2014 Professor Haas was selected as one of ten EPSRCUK RISE Leaders

BiographiesBiographies

Call for Papers

ZTE Communications Special Issue on

Multi1049020Gigabit Millimeter1049020Wave Wireless CommunicationsThe exponential growth of wireless devices in recent years

has motivated the exploration of the millimeterwave frequency spectrum for multi gigabit wireless communications Recent advances in antenna technology RF CMOS processand highspeed baseband signal processing algorithms makemillimeterwave wireless communication feasible The multigigabitpersecond data rate of millimeterwave wireless communication systems will lead to applications in many important scenarios such as WPAN WLAN backhaul for cellular system The frequency bands include 28 GHz 38 GHz45GHz 60GHz EBAND and even beyond 100 GHz Theupcoming special issue of ZTE Communications will presentsome major achievements of the research and developmentin multi gigabit millimeter wave wireless communicationsThe expected publication date will be in December 2016 Itincludes (but not limited to) the following topics

bullChannel characterization and channel modelsbullAntenna technologiesbullMillimeterwavefrontend architectures and circuits

bullBaseband processing algorithms and architecturesbullSystem aspects and applications

Paper SubmissionPlease directly send to eypzhangntuedusg and use the

email subjectldquoZTEMGMMWPaperSubmissionrdquoTentative Schedule

Paper submission deadline June 15 2016Editorial decision August 31 2016Final manuscript September 15 2016

Guest EditorsProf Yueping Zhang Nanyang Technological University

Singapore (eypzhangntuedusg)Prof Ke Guan Beijing Jiao Tong University China

(kguanbjtueducn)Prof Junjun Wang Beihang University China (wangjun

junbuaaeducn)

12