Automated design of microwave discrete tuning differential capacitance circuits in Si-integrated...

6
P opt ¼ 0 in Figure 3(a), it can be seen that the power transfer from the mainline to the subline of the new symmetric design is almost complete as the coupling equals about the insertion loss of 3.5 dB at f 0 ¼ 86 GHz. However, the power transfer is incomplete in the case of the previous design with two coupled asymmetric waveguides in dark state (coupling C 7 dB at f 0 ¼ 103 GHz for P opt ¼ 0). Figure 5 displays experimental results for the mainline trans- mission |s 21 | and the directivity D measured versus frequency for various optical power levels for the new symmetric coupler design. It demonstrates that |s 21 | is efficiently controlled by the laser source over a range of about 15 dB at f 0 ¼ 86 GHz with |s 21 | reaching its maximum value of 11 dB at the highest illumi- nation level P opt ¼ 240 W/cm 2 . Thus, the control range for cou- pling and mainline transmission is quite similar, which makes the device attractive for applications such as a cross-over switch. The directivity of the device is about 20 dB or higher except for intense illumination levels. The reason for the directivity value dropping at intense excitation states is explained by the reflec- tions at the laser-induced plasma layer at the beginning and the end of the active section—cf. curve for |s 11 | in the time domain with P opt ¼ 240 W/cm 2 in Figure 2. 4. CONCLUSIONS A new optically controllable directional coupling structure in image guide technology is proposed with an additional semicon- ductor layer in the active section resulting in a symmetrically horizontally layered device in dark state. By balancing the phase velocities of both the waveguides, a complete power transfer from the input port to the coupled port less the insertion loss of the device can be achieved. The control range for the coupling value versus optical illumination intensity for the device operat- ing in suppression mode—where coupling is reduced with rising optical excitation, whereas the mainline transmission is increased at the same time—has been extended from 7 dB achieved with a previous asymmetric design to 16 dB for the new symmetric structure. Measured coupling values have been confirmed by theoretical results obtained with the effective dielectric constant method. The control range for the mainline transmission is 15 dB and, thus, quite similar to that of the cou- pling value, which makes the device attractive for applications such as a cross-over switch. REFERENCES 1. R. Farias and A. Giarola, Analysis of optically controlled planar dielectric waveguides operating in the millimeter-wave band using FDTD, IEEE Trans Microwave Theory Tech 47 (1999), 639–642. 2. Th. Fickenscher, Optically controlled millimeter-wave parallel guide directional coupler, Asia Pacific Microwave Conference 2008 (APMC 2008), Hong Kong, Conf Proc A2–25, December 2008. 3. M. Tsutsumi and A. Alphones, Optical control of millimeter-waves in the semiconductor waveguide, IEICE Trans Electron E76-C (1993), 175–182. 4. Th. Fickenscher and A. Schwolen, Nonuniform layer model of an image guide millimeter-wave phase shifter, Microwave Opt Tech- nol Lett 41 (2004), 486–490. 5. Th. Fickenscher and A. Schwolen, Experimental verification of nonuniform plasma layer model for quartz-silicon image guide phase shifters, IEEE Trans Microwave Theory Tech 53 (2005), 2375–2382. 6. J.P. Donelly, Limitations on power-transfer efficiency in three guide optical couplers, IEEE J Quantum Electron 22 (1986), 610–616. V C 2010 Wiley Periodicals, Inc. AUTOMATED DESIGN OF MICROWAVE DISCRETE TUNING DIFFERENTIAL CAPACITANCE CIRCUITS IN Si-INTEGRATED TECHNOLOGIES Luı ´s Mendes, 1,2 E. J. Solteiro Pires, 3 Joa ˜o C. Vaz, 2,4 Maria J. Rosa ´ rio, 2,4 P. B. de Moura Oliveira, 3 and J. A. Tenreiro Machado 5 1 Escola Superior de Tecnologia e Gesta ˜ o, Instituto Polite ´ cnico de Leiria, Campus 2, Morro do Lena—Alto do Vieiro, 2411-901 Leiria, Apartado 4163, Portugal; Corresponding author: [email protected] 2 Instituto de Telecomunicac ¸o ˜ es, Instituto Superior Te ´ cnico, Torre Norte, piso 10, Av. Rovisco Pais, no. 1, Lisboa 1049-001, Portugal 3 Centro de Investigac ¸a ˜ o e de Tecnologias Agro-Ambientais e Biolo ´ gicas, Universidade de Tra ´ s-os-Montes e Alto Douro, Quinta de Prados, Vila Real 5000-911, Portugal 4 Instituto Superior Te ´ cnico, Universidade Te ´ cnica de Lisboa, Av. Rovisco Pais, no. 1, Lisboa 1049-001, Portugal 5 Instituto Superior de Engenharia do Porto, Instituto Polite ´ cnico do Porto, Rua Dr. Anto ´ nio Bernardino de Almeida, no. 431, Porto 4200-072, Portugal Received 31 August 2009 ABSTRACT: A genetic algorithm used to design radio-frequency binary-weighted differential switched capacitor arrays (RFDSCAs) is presented in this article. The algorithm provides a set of circuits all having the same maximum performance. This article also describes the design, implementation, and measurements results of a 0.25 lm BiCMOS 3-bit RFDSCA. The experimental results show that the circuit presents the expected performance up to 40 GHz. The similarity between the evolutionary solutions, circuit simulations, and measured results indicates that the genetic synthesis method is a very useful tool for designing optimum performance RFDSCAs. V C 2010 Wiley Periodicals, Inc. Microwave Opt Technol Lett 52: 629–634, 2010; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/ mop.25009 Key words: automated circuit synthesis; genetic algorithms; RF integrated circuits; RF switched capacitor arrays; RF tuned circuits 1. INTRODUCTION The radio-frequency switched capacitor arrays (RFSCAs) have a great potential for use in reconfigurable or adaptive radio-fre- quency (RF) circuits for actual and future wireless transceivers, because they allow a large capacitance tuning range with small tuning steps, when maintaining its quality factor at acceptable values. Moreover, these circuits have no power consumption, which is an important aspect when the transceivers are powered by a battery. At present, RFSCAs can be found in multistandard low-phase-noise ultra-wide-band voltage controlled oscillators [1], in fast-settling time frequency synthesizers [2], in process dispersion compensation techniques [3] and in adaptive imped- ance matching circuits [4]. Optimization and search tools, such as, the genetic algo- rithms (GAs) [5], have been progressively used to automate the design of RF integrated circuits [6–8]. An algorithm to design optimum performance radio-frequency and microwave binary- weighted differential switched capacitor arrays (RFDSCAs) is presented in this article. This new approach, based on e-concept [9] and maximin sorting scheme [10], provides a set of solutions well distributed along an optimal front. Each GA solution that corresponds to a distinct implementation of the desired RFDSCA meets the initial design specifications and has the same maximum performance as the others. This method has bet- ter performance than the one already reported in the scientific DOI 10.1002/mop MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 52, No. 3, March 2010 629

Transcript of Automated design of microwave discrete tuning differential capacitance circuits in Si-integrated...

Page 1: Automated design of microwave discrete tuning differential capacitance circuits in Si-integrated technologies

Popt ¼ 0 in Figure 3(a), it can be seen that the power transfer

from the mainline to the subline of the new symmetric design is

almost complete as the coupling equals about the insertion loss

of 3.5 dB at f0 ¼ 86 GHz. However, the power transfer is

incomplete in the case of the previous design with two coupled

asymmetric waveguides in dark state (coupling C � 7 dB at f0¼ 103 GHz for Popt ¼ 0).

Figure 5 displays experimental results for the mainline trans-

mission |s21| and the directivity D measured versus frequency

for various optical power levels for the new symmetric coupler

design. It demonstrates that |s21| is efficiently controlled by the

laser source over a range of about 15 dB at f0 ¼ 86 GHz with

|s21| reaching its maximum value of 11 dB at the highest illumi-

nation level Popt ¼ 240 W/cm2. Thus, the control range for cou-

pling and mainline transmission is quite similar, which makes

the device attractive for applications such as a cross-over switch.

The directivity of the device is about 20 dB or higher except for

intense illumination levels. The reason for the directivity value

dropping at intense excitation states is explained by the reflec-

tions at the laser-induced plasma layer at the beginning and the

end of the active section—cf. curve for |s11| in the time domain

with Popt ¼ 240 W/cm2 in Figure 2.

4. CONCLUSIONS

A new optically controllable directional coupling structure in

image guide technology is proposed with an additional semicon-

ductor layer in the active section resulting in a symmetrically

horizontally layered device in dark state. By balancing the phase

velocities of both the waveguides, a complete power transfer

from the input port to the coupled port less the insertion loss of

the device can be achieved. The control range for the coupling

value versus optical illumination intensity for the device operat-

ing in suppression mode—where coupling is reduced with rising

optical excitation, whereas the mainline transmission is

increased at the same time—has been extended from 7 dB

achieved with a previous asymmetric design to 16 dB for the

new symmetric structure. Measured coupling values have been

confirmed by theoretical results obtained with the effective

dielectric constant method. The control range for the mainline

transmission is 15 dB and, thus, quite similar to that of the cou-

pling value, which makes the device attractive for applications

such as a cross-over switch.

REFERENCES

1. R. Farias and A. Giarola, Analysis of optically controlled planar

dielectric waveguides operating in the millimeter-wave band using

FDTD, IEEE Trans Microwave Theory Tech 47 (1999), 639–642.

2. Th. Fickenscher, Optically controlled millimeter-wave parallel guide

directional coupler, Asia Pacific Microwave Conference 2008

(APMC 2008), Hong Kong, Conf Proc A2–25, December 2008.

3. M. Tsutsumi and A. Alphones, Optical control of millimeter-waves

in the semiconductor waveguide, IEICE Trans Electron E76-C

(1993), 175–182.

4. Th. Fickenscher and A. Schwolen, Nonuniform layer model of an

image guide millimeter-wave phase shifter, Microwave Opt Tech-

nol Lett 41 (2004), 486–490.

5. Th. Fickenscher and A. Schwolen, Experimental verification of

nonuniform plasma layer model for quartz-silicon image guide

phase shifters, IEEE Trans Microwave Theory Tech 53 (2005),

2375–2382.

6. J.P. Donelly, Limitations on power-transfer efficiency in three

guide optical couplers, IEEE J Quantum Electron 22 (1986),

610–616.

VC 2010 Wiley Periodicals, Inc.

AUTOMATED DESIGN OF MICROWAVEDISCRETE TUNING DIFFERENTIALCAPACITANCE CIRCUITS INSi-INTEGRATED TECHNOLOGIES

Luıs Mendes,1,2 E. J. Solteiro Pires,3 Joao C. Vaz,2,4

Maria J. Rosario,2,4 P. B. de Moura Oliveira,3

and J. A. Tenreiro Machado5

1 Escola Superior de Tecnologia e Gestao, Instituto Politecnico deLeiria, Campus 2, Morro do Lena—Alto do Vieiro, 2411-901 Leiria,Apartado 4163, Portugal; Corresponding author:[email protected] Instituto de Telecomunicacoes, Instituto Superior Tecnico, TorreNorte, piso 10, Av. Rovisco Pais, no. 1, Lisboa 1049-001, Portugal3 Centro de Investigacao e de Tecnologias Agro-Ambientais eBiologicas, Universidade de Tras-os-Montes e Alto Douro, Quintade Prados, Vila Real 5000-911, Portugal4 Instituto Superior Tecnico, Universidade Tecnica de Lisboa, Av.Rovisco Pais, no. 1, Lisboa 1049-001, Portugal5 Instituto Superior de Engenharia do Porto, Instituto Politecnico doPorto, Rua Dr. Antonio Bernardino de Almeida, no. 431, Porto4200-072, Portugal

Received 31 August 2009

ABSTRACT: A genetic algorithm used to design radio-frequencybinary-weighted differential switched capacitor arrays (RFDSCAs) is

presented in this article. The algorithm provides a set of circuits allhaving the same maximum performance. This article also describes thedesign, implementation, and measurements results of a 0.25 lmBiCMOS 3-bit RFDSCA. The experimental results show that the circuitpresents the expected performance up to 40 GHz. The similarity betweenthe evolutionary solutions, circuit simulations, and measured results

indicates that the genetic synthesis method is a very useful tool fordesigning optimum performance RFDSCAs. VC 2010 Wiley Periodicals,

Inc. Microwave Opt Technol Lett 52: 629–634, 2010; Published online

in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/

mop.25009

Key words: automated circuit synthesis; genetic algorithms; RF

integrated circuits; RF switched capacitor arrays; RF tuned circuits

1. INTRODUCTION

The radio-frequency switched capacitor arrays (RFSCAs) have a

great potential for use in reconfigurable or adaptive radio-fre-

quency (RF) circuits for actual and future wireless transceivers,

because they allow a large capacitance tuning range with small

tuning steps, when maintaining its quality factor at acceptable

values. Moreover, these circuits have no power consumption,

which is an important aspect when the transceivers are powered

by a battery. At present, RFSCAs can be found in multistandard

low-phase-noise ultra-wide-band voltage controlled oscillators

[1], in fast-settling time frequency synthesizers [2], in process

dispersion compensation techniques [3] and in adaptive imped-

ance matching circuits [4].

Optimization and search tools, such as, the genetic algo-

rithms (GAs) [5], have been progressively used to automate the

design of RF integrated circuits [6–8]. An algorithm to design

optimum performance radio-frequency and microwave binary-

weighted differential switched capacitor arrays (RFDSCAs) is

presented in this article. This new approach, based on e-concept[9] and maximin sorting scheme [10], provides a set of solutions

well distributed along an optimal front. Each GA solution that

corresponds to a distinct implementation of the desired

RFDSCA meets the initial design specifications and has the

same maximum performance as the others. This method has bet-

ter performance than the one already reported in the scientific

DOI 10.1002/mop MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 52, No. 3, March 2010 629

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literature [11], because it reduces substantially the solutions dis-

persion along the optimum front. The reported method, based on

sharing scheme [12], presents a poor solutions distribution and,

consequently, an undefined front.

To provide a better insight into the design of RFDSCAs with

optimum performance, a case study is presented. Bearing this

idea in mind, all the design steps, including the specifications,

circuit synthesis, SpectreRF simulations, implementation, and

measurements, are performed. The design used a 0.25 lm BiC-

MOS technology. The measurement results demonstrate that the

implemented 3-bit RFDSCA has a high minimum quality factor

and presents the expected performance up to 40 GHz. The simi-

larity between the evolutionary solutions, circuit simulations,

and measured results clearly shows that the proposed RFDSCA

synthesis procedure constitutes a very powerful design tool.

This article is divided in four sections. Section 2 presents the

behavior model of the RFDSCAs, the developed GA, which is

used to synthesize several RFDSCA circuits, and the design

steps that must be followed to implement successfully an opti-

mum performance RFDSCA. Section 3 presents a case study,

namely, the design, simulation, implementation, and measure-

ments results of a microwave RFDSCA. Finally, Section 4

draws some conclusions.

2. RFDSCA DESIGN PROCEDURE

This section describes in detail the automated synthesis proce-

dure adopted for designing optimum performance RFDSCAs. In

this sense, it begins by presenting the closed-form mathematical

expressions that characterize the RFDSCA behavior. After that,

the developed GA, which is the core of the automated design

procedure, is described. Finally, the section ends with the enu-

meration of the required steps that should be followed to design

successfully an optimum performance RFDSCA.

2.1. The RFDSCA Behavior ModelThe simplified circuit of a RFDSCA is illustrated in Figure 1.

This schematic has a similar topology to the one reported in

[11]. The changes introduced in the single-ended RFSCAs

model were done to account for the use of a differential topol-

ogy. Figure 1 shows that the RFDSCA circuit can be divided in

N different cells. The first cell, which is the reference cell, com-

prises two reference capacitors with value C and a reference

switch. The other cells of the RFDSCA are constituted by two

cell capacitors and a cell switch. The capacitance value of the

cell capacitors is equal to 2k�1�C and the number of reference

switches of each cell is given by 2k�1 (k is the number of the

cell, 1 < k � N). Figure 1 also shows that the reference switch

is formed by placing in parallel M basic switches (BS).

The BS, implemented with MOS transistors, has two domi-

nant sources of loss: the channel resistance when the transistors

operate in the deep triode region, RBS-ON (BS-ON) (Fig. 2), and

the substrate resistance when the transistors are in cut-off

region, Rsub (BS-OFF) (Fig. 3). Both resistances limit the maxi-

mum achievable quality factor of the RFDSCA (QRFDSCA). Fur-

thermore, in the cut-off region, it is important to consider the

substrate-drain junction capacitance, CsubD, the substrate-source

junction capacitance, CsubS, the gate-drain capacitance, CGD, and

the gate-source capacitance, CGS, because these elements have a

major impact upon the RFDSCA minimum capacitance and the

maximum attainable QRFDSCA. Taking into account the aforesaid

considerations and the NMOS physical model represented in

Figures 2 and 3 [13], the simplified BS model for the ON and

OFF states can be represented by the equivalent circuits of Fig-

ures 2 and 3 [14] [15], respectively. Note that the BS-ON resist-

ance, RBS-ON, the BS-OFF resistance, RBS-OFF, and the BS-OFF

capacitance, CBS-OFF, are highly dependent on the fabrication

process, layout, and bias conditions.

The RFDSCA can be modeled as a nonideal controlled ca-

pacitor. The RFDSCA input admittance can be described by the

following:

�YRFDSCAðD; f Þ ¼ 1

RRFDSCAðD; f Þ þ j � 2 � p � f � CRFDSCAðD; f Þ;(1)

where CRFDSCA and RRFDSCA represent the RFDSCA equivalent

parallel capacitance and resistance, respectively. In this equa-

tion, D is the control word and f represents the operating fre-

quency. The control word D ¼ bN�2N�1 þ…þ b2�21 þ b1�20 is

the decimal representation of the binary word [bN … b2 b1]

Figure 1 Generic RFDSCA schematic

Figure 2 Basic switch model: ON state. [Color figure can be viewed

in the online issue, which is available at www.interscience.wiley.com]

Figure 3 Basic switch model: OFF state. [Color figure can be viewed

in the online issue, which is available at www.interscience.wiley.com]

630 MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 52, No. 3, March 2010 DOI 10.1002/mop

Page 3: Automated design of microwave discrete tuning differential capacitance circuits in Si-integrated technologies

(control bits). This relation is fundamental in the following anal-

ysis, because the closed-form mathematical expressions use D as

an independent variable. Moreover, DMAX ¼ 2N � 1 corre-

sponds to the maximum value of D.It can be demonstrated, considering the RFDSCA topology

and the BS equivalent circuit, that the equivalent capacitance

and quality factor of the RFDSCA are expressed by (2) and (3),

respectively.

CRFDSCAðD; f Þ ¼D � C

2þ DMAX �M � CBS�OFF

1þ 2�M�CBS�OFF

C

þ 0 � f (2)

QRFDSCAðD; f Þ ¼1þ2�M�CBS�OFF

Cð Þ� 1þ DDMAX

� C2�M�CBS�OFF

� �2�p�f �RBS�OFF �CBS�OFF

1þ DDMAX

� C2�M�CBS�OFF

þ 1� �2

� RBS�ON

RBS�OFF� 1

� � (3)

The RFDSCA model is based on six design parameters and

two independent variables (D and f). The design parameters that

can be optimized to obtain a RFDSCA with optimum perform-

ance are N, M, and C, because RBS-ON, RBS-OFF, and CBS-OFF are

defined by the integration technology and bias conditions. Thus,

any RFDSCA circuit can be fully defined by the variables N, M,

and C. Besides that, Eqs. (2) and (3) are crucial to the RFDSCA

design algorithm because they are used during the automated

synthesis procedure to verify the initial specifications and to

evaluate the performance of each solution, as it will be

explained in the next two subsections.

2.2. Optimization AlgorithmThe automatic design synthesis procedure uses a GA to generate

several RFDSCA circuits that meet the design specifications, all

with identical maximum performance (given by the quality fac-

tor). Each GA solution, that corresponds to a specific RFDSCA

circuit, is defined by the N, M, and C. The developed GA,

which is described by the flowchart of Figure 4, uses the e-con-cept and the maximin sorting scheme to guarantee that the gen-

erated solutions are spread along an optimal front in the parame-

ter space. The e-dominance allows keeping a solution front in

the search space over evolution and the maximin technique pro-

motes the diversity along each generation.

The flowchart of Figure 4, apart from the maximin selection

step, represents a standard GA. It begins by randomly initializ-

ing the population P(t), where variable t identifies the genera-

tion, videlicet, the GA cycle number. Each individual of the

population (potential solution/circuit) is represented by pi(t) ¼{Ni, Mi, Ci} where Ni, Mi, and Ci are the number of cells, num-

ber of BSs, and the value of the reference capacitances for the

individual i, respectively. The algorithm uses a population of

1000 individuals (the maximum value of i is 1000). The floating

point values of Ni, Mi, and Ci are randomly initialized (at t ¼ 0)

in an appropriate range (Ni ¼ 1 … 64, Mi ¼ 1 … 64, and Ci ¼1 fF … 1 pF). The search is then carried out within this popula-

tion over 105 generations (the maximum value of t is 105). Afterthe initialization, a fitness value (fv) for each population element

is evaluated in order to determine the solution performance. The

evaluation of fv leads to a positive value equal to 2�p�f�QRFDSCA

if the solution verifies all the design specifications, otherwise it

takes a negative value according to the distance to the feasible

space. Then, the selection operator, based on the linear ranking

scheme, is used to identify the most capable parents to generate

proficient offspring (set D(t)). To create individuals with new

genetic material, the operators simulated binary crossover and

mutation are used. When mutation occurs, the operator replaces

the value of each individual chromosome according to a uniform

distribution function. The uniform function varies in the range

[�Ui, Ui] where Ui ¼ {0.2, 0.2, 0.4 � 10�15} for Ni, Mi, and

Ci, respectively. The crossover and mutation probabilities are pc¼ 0.6 and pm ¼ 0.05, respectively. In the following step, the fit-

ness of each element of the population is again calculated and

the maximin technique is applied to disperse the solutions over

a continuous front. The cycle is repeated until the predefined

maximum number of iterations is reached (t ¼ 105).

2.3. Design StepsThe simplified flowchart of the RFDSCA design procedure is

depicted in Figure 5. The first design step comprises two

actions. One action is the specification of the desired perform-

ance characteristics of the RFDSCA, which are defined by the

maximum capacitance, CMAX, minimum capacitance, CMIN, and

the tuning capacitance step, DC. These three values impose the

bounds for the RFDSCA capacitance. The other action consists

in the definition of the technology design variables RBS-ON,

Figure 4 Flowchart of the genetic algorithm

Figure 5 Flowchart of the RFDSCA design algorithm

DOI 10.1002/mop MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 52, No. 3, March 2010 631

Page 4: Automated design of microwave discrete tuning differential capacitance circuits in Si-integrated technologies

RBS-OFF, and CBS-OFF, which can be determined from the Si-inte-

gration technology process parameters and models.

The second design step is the execution of the proposed GA.

For that, it is necessary to define the design restrictions and the

fitness function appropriated for this type of circuits. The design

restrictions that are related to the initial RFDSCA specifications

are defined by the three inequalities given in (4):

CRFDSCA�MAX � CMAX

CRFDSCA�MIN � CMIN

DCRFDSCA � DC

8<: (4)

In (4) CRFDSCA-MAX, CRFDSCA-MIN, and DCRFDSCA represent

the maximum RFDSCA capacitance, the minimum RFDSCA ca-

pacitance, and the RFDSCA tuning capacitance step, respec-

tively. These three values are determined by the GA from

expression (2). To achieve high performance RFDSCAs, it is

necessary to determine the number of cells and the components

values and sizes that maximize the RFDSCA quality factor. Not-

ing that QRFDSCA decreases monotonically with f (see (3)), the

objective function for this kind of RF circuits can be made inde-

pendent of it. Therefore, the chosen optimization objective func-

tion is given by expression (5):

fvðDÞ ¼ 2 � p � f � QRFDSCAðD; f Þ (5)

The outcome of the GA is a set of several RFDSCA circuits,

each one defined by specific values of N, M, and C, all having

identical performance. The next step in the RFDSCA design

procedure consists in choosing the circuit that is best suited to

be implemented in a particular Si-integration technology. This

action is done by the designer. As a general design rule, the cir-

cuit that should be implemented is the one that has the lower

number of cells, because this allows minimizing the number of

control variables and, in certain cases, the parasitic elements

associated to the interconnections. The design procedure ends

with the circuit tape-out.

3. A RFDSCA DESIGN CASE STUDY

This section presents the design and measurement results of an

optimum performance RFDSCA, intended for applications that

operate at frequencies up to 40 GHz. The design is accom-

plished using the home made automated synthesis procedure

previously described.

3.1. Specifications, Design, and SimulationThe objective is to implement a microwave discrete tuning dif-

ferential capacitance circuit in a 0.25 lm BiCMOS technology.

The RFDSCA should present at least a minimum capacitance of

CMIN ¼ 72 fF, a maximum capacitance of CMAX ¼ 108 fF, and

a maximum tuning step of DC ¼ 8 fF, as indicated in (4).

Besides that, the quality factor of the RFDSCA should be as

high as possible.

The differential BS is made up of a single NMOS transistor,

with length of 0.25 lm and width of 720 nm, which corresponds

to the minimum dimensions provided by the BiCMOS integra-

tion technology. Considering the SPICE models of the transis-

tors and the technological process parameters, the elements of

the BS model are those given in (6):

Figure 6 Automated synthesis results: M and C versus N. [Color fig-

ure can be viewed in the online issue, which is available at www.

interscience.wiley.com]

Figure 7 Die photomicrograph. [Color figure can be viewed in the

online issue, which is available at www.interscience.wiley.com]

TABLE 1 RFDSCA Performance Results

Circuit Type of Results N M C (fF)

Design Constraints

CRFDSCA-MAX (fF)

(�108 fF)

CRFDSCA-MIN (fF)

(�72 fF)

DCRFDSCA (fF)

(�8 fF)

Cir1 Genetic algorithm 2.998 5.026 30.93 108 71.95 5.185

SpectreRF (schematic) 3 5 30.9 108 71.70 5.185

Cir2 Genetic algorithm 4.0011 2.3476 14.40 108 71.90 2.408

SpectreRF (schematic) 4 2 14.40 108 67.92 2.670

Cir3 Genetic algorithm 4.998 1.1251 6.99 108 71.65 1.179

SpectreRF (schematic) 5 1 6.97 108 68.74 1.265

632 MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 52, No. 3, March 2010 DOI 10.1002/mop

Page 5: Automated design of microwave discrete tuning differential capacitance circuits in Si-integrated technologies

RBS�ON ¼ 73:6X ð@VGS ¼ 3VÞRBS�OFF ¼ 18:9X ð@VGS ¼ 0VÞCBS�OFF ¼ 6:1fF ð@VGS ¼ 0VÞ

8<: (6)

These values are almost constant in the frequency range

from 1 to 40 GHz.

The values of the six design variables specified in (4) and (6)

are the only ones that must be known before running the

RFDSCAs synthesis method. The solutions found by the auto-

mated synthesis procedure are represented in the two curves of

Figure 6, where the red one presents M versus N (curve marked

with the þ symbol) and the blue corresponds to C versus N(curve marked with the (symbol). Moreover, all the circuits gen-

erated by the algorithm reveal an high performance because the

minimum QRFDSCA at 15 GHz, calculated by the GA, is �47.

To find an optimum performance RFDSCA circuit, it is only

necessary to select the appropriate value of N, because M and Care immediately defined by this value. Figure 6 also shows that

the algorithm finds a well-defined front with good diversity.

Moreover, the results obtained show that the algorithm conver-

gence ability is very good because all the solutions are in the

nondominated front.

To verify the solutions provided by the RFDSCAs synthesis

procedure, three different circuits were chosen and simulated in

SpectreRF. These are identified as Cir1, Cir2, and Cir3 in Figure

6 and in Table 1. The results of Table 1 show that the values of

CRFDSCA-MAX, CRFDSCA-MIN, and DCRFDSCA obtained through

the SpectreRF schematic simulations of the three circuits are

similar to those achieved with the GA. Moreover, the simulated

circuits meet all the design constraints.

3.2. Implementation and Experimental ResultsTo verify, in practice, the performance of the design procedure,

one RFDSCA was implemented and tested. The circuit Cir1 of

Table 1 was chosen to be implemented and tested, because it is

the one that requires the lower number of cells.

To improve the similarity between the calculated, simulated,

and experimental results some valuable techniques can be used

during the RFDSCA layout design. Parasitic elements are an im-

portant issue, because the RFDSCA performance is extremely

sensitive to them. Thus, the interconnection lines should be as

short as possible in order to reduce their parasitic resistance, ca-

pacitance, and inductance. The cross line also must be avoided,

to reduce the parasitic capacitance. Furthermore, too thin or too

wide lines are not recommended, because they will produce

large parasitic resistance or capacitance, respectively. The inter-

connecting resistance is further reduced by using the topmost

metal layer, due to low resistivity, or by stacking the top two

metal layers. All the above considerations were taken into

account when laying out the RFDSCA.

Figure 7 depicts the photomicrograph of the implemented

RFDSCA. The differential input is identified by the IN-P and

IN-N pads and the control bits by the b1, b2, and b3 pads. The

circuit size, excluding the pads, is 0.0256 mm2. The RFDSCA

was measured on-wafer using a Cascade Summit 9000 probe

station, two 40 GHz Cascade Infinity ground-signal-ground

probes and a 67 GHz Agilent PNA network analyzer (E8361A).

The SpectreRF schematic and post-layout simulations and

the experimental results of Cir1 are shown in Table 2. The

measured results presented in this table are obtained after de-

embedding the effects of the auxiliary measure structures, in

other words, after removing the parasitic resistances, capacitan-

ces, and inductances associated to the interconnections between

the probes and the RFDSCA circuit. The differences between

the schematic and the pos-layout simulations results are funda-

mentally due to the parasitics associated to the RFDSCA metal

interconnections, because the major differences occur only in

the extreme values of the capacitive tuning range. The simula-

tion results of Table 2 show that these differences come from a

constant parasitic capacitance of 39 fF, which is also independ-

ent of the tuning word. The RFDSCA measured results pre-

sented in Table 2 show that the implemented version of Cir1

has a performance very similar to the one obtained by the pos-

layout simulations. Besides that, the RFDSCA capacitance for

each tuning word is almost constant in the frequency range of

1–40 GHz, as illustrated in Figure 8.

4. CONCLUSIONS

This article presents a RFDSCA automated synthesis procedure.

This algorithm determines several RFDSCA circuits, all with the

same maximum performance, from the top-level system specifi-

cations. The genetic synthesis tool optimizes a fitness function

proportional to the RFDSCA quality factor and uses the e-con-cept and maximin sorting scheme to achieve a set of solutions

well distributed along a nondominated front. To verify the

results of the algorithm, three RFDSCAs were simulated in

SpectreRF and one of them was implemented and tested. The

design used a 0.25 lm BiCMOS process. All the synthesized,

simulated, and measured results were very close.

ACKNOWLEDGMENTS

The authors thank the Instituto de Telecomunicacoes for funding

this project IT/LA/304/2005.

TABLE 2 Cir1 Performance Results

Cir1 Results

Design Constraints

CRFDSCA-MAX

(fF)

CRFDSCA-MIN

(fF)

DCRFDSCA

(fF)

SpectreRF

(schematic)

108 71.70 5.185

SpectreRF

(post-layout)

147 111 5.14

Measured

(after

de-embedding)

�148@15 GHz �116@15 GHz �4.57@15 GHz

Figure 8 Measured RFDSCA capacitance versus frequency for all the

tuning words

DOI 10.1002/mop MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 52, No. 3, March 2010 633

Page 6: Automated design of microwave discrete tuning differential capacitance circuits in Si-integrated technologies

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VC 2010 Wiley Periodicals, Inc.

LINEARIZATION OF A 3.7 GHzMULTI-CARRIER GaN HEMT DOHERTYPOWER AMPLIFIER USING DIGITALPREDISTORTION METHOD

Jonghyuk Jeong, Juho Van, Jaeyong Cho, Min-Su Kim,Hanjin Cho, Kyung-Hoon Lim, Sung-Wook Kwon,Kyonggon Choi, Hyung-Chul Kim, Sungcheol Yoo,Cheon-Seok Park, and Youngoo YangSchool of Information and Communication Engineering,Sungkyunkwan University, Suwon, Korea; Corresponding author:[email protected]

Received 17 August 2009

ABSTRACT: In this article, a 3.7 GHz band Doherty amplifier basedon GaN HEMTs, which is linearized using a digital predistortionmethod, is implemented for 4th generation wireless communication

systems. The forward and reverse models of the Doherty amplifier forthe predistortion consist of simple polynomials whose coefficients are

extracted using a conventional least mean square error algorithm. Usinga two carrier signal based on IEEE802.16e, whose PAR is 9.44 dB, an

ACLR improvement of 10.74 dB is achieved to give an ACLR level of41.74 dBc at an offset of 4.79 MHz. The overall efficiency of theDoherty power amplifier is 13.74%, which represents a 2.44%

improvement compared with that of a balanced class-AB poweramplifier at an average output power of 36 dBm. VC 2010 Wiley

Periodicals, Inc. Microwave Opt Technol Lett 52: 634–638, 2010;

Published online in Wiley InterScience (www.interscience.wiley.com).

DOI 10.1002/mop.24984

Key words: power amplifier; Doherty amplifier; GaN HEMT; digital

predistortion; linearization

1. INTRODUCTION

Both linearity and efficiency are important performance meas-

ures for RF power amplifiers, because the performance of the

transmitter system is determined by that of the power amplifier

[1–6]. Especially, for the upcoming 4th generation wireless sys-

tems, it is necessary to use a higher peak-to-average power ratio

(PAR) and higher frequency operation of the digital-modulated

signals. Therefore, it becomes harder to secure very good linear-

ity and efficiency at the same time.

As it has a high efficiency over a wide output power range,

the Doherty power amplifier has been widely used for various

wireless communication systems [1, 2]. However, the Doherty

amplifier needs to be linearized using additional circuits or sys-

tems, such as feedforward or digital predistortion methods, due

to the stringent linearity requirements of the base transceiver or

relay systems. The digital predistortion method has advantages

in comparable linearization techniques due to its low cost imple-

mentation and high efficiency of operation compared with the

feedforward technique [4, 5].

In this article, high efficiency Doherty power amplifier based

on GaN HEMTs for 3.7 GHz 4th generation wireless systems is

implemented and its performance compared before and after lin-

earization; a conventional class-AB amplifier has also been built

using the same device configuration [6].

Full simulation procedures and their results are included for

the digital predistortion. The forward and reverse polynomial

models for both the amplitude-to-amplitude (AM–AM) and am-

plitude-to-phase (AM–PM) characteristics of the power amplifier

have been built based on the measured baseband input and

output signals of the power amplifier. The reverse polynomial

models for both the AM–AM and AM–PM characteristics are

applied for the digital predistorter. Simulations have been

carried out for the digital predistortion to predict the lineariza-

tion performance for the implemented Doherty amplifier in

MATLAB.

Figure 1 A schematic diagram of the Doherty power amplifier. [Color

figure can be viewed in the online issue, which is available at

www.interscience.wiley.com]

634 MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 52, No. 3, March 2010 DOI 10.1002/mop