Chapter 10shodhganga.inflibnet.ac.in/bitstream/10603/23054/... · Chapter 10 OTA-based Analog...

28
Chapter 10 OTA-based Analog Multiplier 1 O.J Introduction In this chapter application of OTA as a multiplier is presented. Analog multiplier plays un imponnnt role in analog signal processing system. In this chapter lir.;t n review of different analog multiplier architectures, which have been proposed over the Inst fillecn year:,, is given. Few low-power multiplier structures simulated in Cadence Virtuoso Design cnvirowneni to obtain their characteristics such as input range, linearity. input noise and power consumption. The new structure is proposed for the unn log multiplier using cross-coupled OT A that has low power dissipation while at the same time keeping good linearity, low supply voltage and low noise. The quantitative analysis on linearity, power consumption and noise for proposed multiplier is also presented, which is verified by Spectre Simulatot from Cadence tools [69-71 ). Simulation results showed that the proposed multipli er is showing good performance. 10.2 Ana l og Multiplier Real time analog multiplication of two signals is one of the most imporlam operations in analog signal processing. /\. multiplier is an active network. lhe output of which is proportional to the product of two input signals. A general rcprcscnlation of multiplier is Z= K. X.Y ( 10.1) 136

Transcript of Chapter 10shodhganga.inflibnet.ac.in/bitstream/10603/23054/... · Chapter 10 OTA-based Analog...

Page 1: Chapter 10shodhganga.inflibnet.ac.in/bitstream/10603/23054/... · Chapter 10 OTA-based Analog Multiplier 1 O.J Introduction In this chapter application of OTA as a multiplier is presented.

Chapter 10

OTA-based Analog Multiplier

1 O.J Introduction

In this chapter application of OTA as a multiplier is presented. Analog multiplier

plays un imponnnt role in analog signal processing system. In this chapter lir.;t n review

of different analog multiplier architectures, which have been proposed over the Inst

fillecn year:,, is given. Few low-power multiplier structures an~ simulated in Cadence

Virtuoso Design cnvirowneni to obtain their characteristics such as input range, linearity.

input noise and power consumption.

The new structure is proposed for the unnlog multiplier using cross-coupled OT A

that has low power dissipation while at the same time keeping good linearity, low supply

voltage and low noise. The quantitative analysis on linearity, power consumption and

noise for proposed multiplier is also presented, which is verified by Spectre Simulatot

from Cadence tools [69-71 ). Simulation results showed that the proposed multiplier is

showing good performance.

10.2 Analog Multiplier

Real time analog multiplication of two signals is one of the most imporlam

operations in analog signal processing. /\. multiplier is an active network. lhe output of

which is proportional to the product of two input signals. A general rcprcscnlation of

multiplier is

Z= K. X.Y ( 10.1)

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where X and Y are the two input signals with K being multiplier constant with

suitable dimensions. All signals, i.e. X, Y and Z are measured with respect to ground.

The signals can be either voltages or currents.

The multiplier is used not only as a computational building block but also as a

programming element in systems such us filte~. neural networks und as mixer and

modulators in communication systems. Verities of multipliers have been designed for

different objectives and some of them are driven by the early work of Gilbert (71-73]. A

general idea behind these designs is to use electronic devices to process input signals in

analog domain, followed by cancellation or minimization of error caused by non-linearity

of devices. Tht: CMOS multiplier implementation is sti ll a challenging subject especially

for low-voltage and low power coni;umption (71 ).

10.2.1 Basic Idea of Multiplier

The basic idea of multiplier implementation is illustrated in Fig.10.1. Two signals

v,(t) nnd vz(t) urc upplled to nonlinear device, which can be characterized by a high order

polynomial function. This polynomials function generates second order, third order and

many others tenns beside the desired v1(t).v2(t). Then it is required to cancel the

undesired components. This is accomplished by a cancellation circuit configuration. The

differential ci rcuit structure is widely used for nonlinearity cancellation [71) .

..------- "\

Nonlinur Device

i.e.,

;0 = av, +bv,2

+cv,>+/\

Nonlinearity i., = /cv1 (t )v1 (t)

cancellation scheme

Figure 10.1 Basic idea of multiplier

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For a multiplier circuit with two inputs there are four combinations of two

diff1::rcntial signal::;, i.e., (x, y), (-x, y), (X, -y), (-x, -y). Two example topologies for

multiplier implementalion are shown in Fig.10.2 [71].

x+y I 2 l x + xy+ y

x 2 2 ,

·x+y x - xy+y

I l x +2xy+ y

l 2 l x - xyt y

(u) (b)

Figurel0.2 Example topologies to implement analog multiplier structures

The topologies, shown in Fig. I 0.2, achieve multiplication and simultaneously

cancel out all the higher order and common-mode components (X and Y) based on the

relation (10.2) for Fig. 10.2(a) and relation (10.3) for Fig. 10.2(b) (x and y represent

small signals).

[(X+x)(Y+y) + (X-x)(Y-y)]- [(X-x)(Y+y) + (X+x)(Y-y)] = 4x.y (I 0.2)

[ {(X+x) + (Y+y)}2 + {(X-x) + (Y-y)} 2] - [ {(X-x) + (Y+y)} 2 + {(X+x) + (Y-y)}

2]

= 8x.y (10.3)

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10.3 CMOS Multiplier

As th~ digital technology dominates in modem electronics, 3nalog 1,;ircuits are

required to use the same standard CMOS process for low-cost fabrication. Due to the

popularity of advanced CMOS technology, with 1,;mphosis on low power consumption,

MOS transistors are a natural choice for the devices, while differential circuit is widely

used for non-linearity cancellation [73J. For CMOS analog multiplier des ign, the simple

MOS transistor model is expressed as relation (I 0.4) and ( I 0.5).

Id= K [Vos- Vr- Vos/2]Vos for Yvs >Yr, Vos < Yes- Yr ( 10.4)

for VGs >Yr, Vos> Yes- VT (I 0.5)

For MOS in its linear nnd saturation region, respectively, K ""µo. Cox (W/L) and

VT are the conventional for the transconductance par3mctcr and threshold voltngc of the

MOS trans istor, respectively. Fig. 10.3 shows the application methods for two signals (x

and y) in a MOSFET. Jn Fig. 10.3 the small circle on the transistor terminal represents a

fixed biasing voltage, x and y are time-variable voltage signals, disregarding the bins [711.

The first three methods are used for MOSFET's operating in their linear region and the

rest are for transistors operating in saturation. The signal injection methods (b), (d) and

(g) in Fig. 10.3 require a voltage summing circuit. This voltage summation can be

implemc:111c:d in different ways, ulthough the perfonnancc of the swruncr directly affects the

perfonnance of multiplier [71].

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±y ±.x±y ±r~ ±x±y

:!:x-l~y ~~;· ~;. ±y-f

(a) (b) (c) (d)

sli. f ±x-i ~id :tx4 ±x±y-1 ±y

(e) (f) (g)

Figure 10.3 Voltage signals injection methods

10.3.1 Multiplier Characteris tics

Accuracy: Accuracy is specified as the deviation of the actual output from char of ideal,

for any combination of X and Y input within the specified operating range of the

multiplier r73J.

Linearity: The accuracy of multiplier is usually expressed in term of its linearity. A

graph of output voltage as function of one of the input voltage is obtained, with the other

input voltage kept at some constant value. The input voltage that is kept constant is

usually set to its maximum or full-range value. Linearity is most commonly defined as

the maximum percentage deviation from ''best straight line" data at the output,

corresponding to equal magnitude input at the X and Y terminals.

Linearity error is plotted dilTerent for X and Y input, when these plots are

combined, they present an error surface. Hence linearity error can also be defined as the

maximum absolute deviation of the error surface. Some time linearity error is also

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defined as a pt:rccntage of full-scale output, as the maximum devintion from linearity

occun-cd at lhc extreme;: t:nd of multiplier dynamic range as shown in relntion (10.6).

Linearity Error "' (6 Vz I Vz tr.ti ... 1,>I (10.6)

where 6 Vz - actual value;: uf oucput - expected value of output and Vz is output voltage

of multiplier. Linearity error cannot be reduced and places a lower limit on multiplier

accuracy.

Quadrant: This indicate~ whether the device will accept bipolar signal. If it accepts only

positive signals, it is a First quadrant: if it accepts only one bipolar signal, it is Two

quadrants; if it accepts two bipolar signals, it is a Fnur quadrant dc::vicc.

Scale Factor: Scale factor is defined to be the proportionality constant, relating the

output voltage and the product of the input voltages as given in relation (I 0. 7).

K=Z / XY ( 10.7)

ln equation (10. 7), K is found at particular value of X, Y and Z.

The measurement of multiplier performance can include input range, linearity,

power consumption, &equency range, and noise and so on. Since all these performance

measure are strongly application dependent, there is not an absolute standard comparison

metric. Also, it is not wicommon that some metrics need to be tru.dcd for other. for

instance, as the power consumption of multiplier is lo be optimized, its linearity gets

worse. This required reasonable tradeoff between the two. Herc the attempt is made to

compare three multipli~r structures according to different criteria such as input range,

linearity, noise and power consumption etc [73).

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l 0.4 Common Multiplier Structures

This section includes comparative study of some common multiplier strucrur~s

proposed in f7 I]. Fig. I 0.4 shows 1hcsc: mulliplicrs structures.

Y+y-1 t-Y+y

X-x x+x X-x

(a) (b)

X+x

(c)

(d) (c)

Figure 10.4 Common multiplier Structures

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These five multipliers havo been des igned without considering a specific

performance for rough comparisons [71]. The circuit of Fig.10.4 (b) and (c) have low

transconductance. The multiplier circuit of Fig. I 0.4 ( e) signifi cantly consumes higher

power than any other circuits. The output current of circuit Fig. I 0.4 (b) and Fig. 10.4(c)

have high sensitivity on device mismatch. From complexity of circuit topologies

conclusion is (71]

• the circuit Fig. I 0.4 (b) has low transconductance, is sensitive to mismatch, and

has poor linearity

• Lhe circuit Fig. l 0.4 (c) is sensitive to mismatch anel has low transconduclance

• tin~ circuit Fig. l 0.4 (e) con!;umcs high power and has poor linearity

The linearity of circuit Fig. I 0.4 (a) improves as the source follower use larger

W/L ratio. This effect is not clear in the case of circuit Fig.10.4 (<.I). For the !;ame input

range and output node voltage swing, circuit Fig. l 0.4 (a) requires lower power supply

than Fig.10.4 ( d). So multiplier structure of Fig. I 0.4 (a) seems to be most attractive

structure for low voltage and low power applications, also has good performmce metrics

as compared to other structures [71). In this thesis the two architectures (Fig.10.4 (a) and

fig. I 0.4 (b)) were simulated using Cadence's Custom lC Design Tools in 0.35um CMOS

technology with process parameters given in table 7.1 and their performance was

compared to with the multiplier, proposed in this thesis. These structures arc called as

structure I and structure II in this thesis.

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t 0.4.1 Multiplier Structure I

Fig.10.5 shows multiplier structure I, which is the most recom1mmdcd multiplier

structun:, provided in L 71].

Figure 10.S Multiplier s tructure I

A folly differential configuration improves the linearity because a better non­

linearity cancellation is achieved. The folly differtmtinl configuration using four MOS

transistor i.e., N l - N4 operating in linear region and upper four MOS transistor i.e., Ml

- M5 are operated in saturation region. For the cin.:uit shown in Fig. I 0.5, the differential

output current is given by equation (10.8) which gives the multiplication of two signals.

l ou• = 101 - 102 = lout - K [((Vy+ ZVx) 2

- (Vy · 2Vx) 2] ~lout= 4 K VxVy (10.8)

10.4.1.1 Input Range

The input range of a multiplier circuit is obtained from its bias conditions.

Constraint set ( I 0.9) gives the required bias conditions for the structure I.

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VT < X :!: x

vi= Y ± Y - vT VT< y ± y

y ± y - Vr < V4

l 0.4.1.2 Linearity Analysis

< x ± x - VT

( 10.9)

!'ht: DC transfers characteristics of (lo1- Io2) versus x and y is shown in Fig. 10.6 (a)

and (b). A DC transfer characteristic shows that the structure in Fig. I 0.5 is four-quadrant

multiplier. The structun.:: is able to accept two bipolar signals as input.

,,.., ...

Su •· •••

6u ·· .......

···. H- 0~ ......... ~

-· .. ....... ···

4u ......... • •• •..••

~II •· ............ .......... '• ••• ., • •. • ,. •••• •••• ••••••• - ······· ,_. - •·

i .:.. ···········-·· .. ······- .... -.: ... :::::::~~~;/!=:··· .. (=:::::~::::·::: .. -~- .:: ...... .

.,., .....

.................. ......

·····-···········

~ ·· •..

· I 0<'.0·'"=2------0 I ----~O~------,O~l-­)11")

·~ . ,__, 0 2

Figure 10.6 (a) DC trun~fcr churn<:tcrbth.::s l out versus y for Structure I

The linearity error versus y and x inputs is shown in Fig. 10. 7 (a) and (b)

respectively. The linearity error increased as the value of both x and y inputs increases. In

particular, when x= 0.12 and y=0.2V, the linearity error is measured to be 4.8 % and

when x = 0.2V and y = 0.12V, the linearity error is measured to be 0.89 %.

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I OU f S u .

!

6u 1 .tu ;

.-,.. ~u f ~o[ lS ~

- - :?u t

~·= - ( t.:

4 u i . · Gu l r=u.:?

!

-811 i.

-!Ou !. ~.:_. -----· -0. ~

Figure 10.6 (b) DC tr:ansfer characteristics l 0 u1 v ersus x for structure I

Linearity Error

6 ---- ---- ----·- - - ---- -------- -------------- !

5 +--- -----------------------;! _,...--------------... ~ 4 +--- ----,--"'"----- -- - ---- --- ------.., ~ /,.---' ~ 3 +----"7"------------------; ·E • ~ 2 +------------------- ----l

:.:J

0 +---- --,--------.---------,-------; ODB 0 .12 0 .16

X• 0.2V y(v)

Figure 10.7 (a) Linearity Error versus y for structure I

1

0 .9 * 0 .6 ':::"' 0 .7

.E 0 .6 ~ 0 .5 ·.., 0 .4 ~ 0 .3

:.:J 0 .2 0 .1

0 o.c ~

Linearity Error

------· ___ .. --- ----

0 .08 0 .12 0 .16

x(v)

Figure 10.7 (b) Linearity Error versus x for structure I

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The Total Hannonic Distortion (THD) is calculated when a constant DC voltage

is applied to x (or y) while a 100 KHz 0.2Vp-p sinusoidal wave is applied to y (or x) [73)

is shown in Fig.10.8 (a) and (b).

THO

8 7

ae .. 8 !5 ---t 8.< -----~ 8 3 --8 2 8.1

8

;9 o~ 0' 0 1 ~ 0 2

! IV i

Figure 10.8 (a) THD of signal y with x == 0.2 V for structure I

THO

3

2. ~

~ 2 -

~ 1 5

~ 1

0.5

~

o o~ 0 1 o ,e o: x (v;

Figure 10.8 (b) THD of output signal with y = 0.2V for structure I

Fig.10.8 (a) and (b) shows the multiplier has good linearity with respect to x input.

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10.4.1.3 Power Consumption

for given constant power supply, the power consumption of multiplier can be

estimated by looking at the total supply voltage (Vdd) current, which is given by relation

(10.10).

(1 0.10)

I..,..,1 - (K,10/2)[ Y -y-V ut - Vr]2 + (K,..n/2)( Y-y- Y 112 - VrJ2 + (K MJl2)(Y+y- V a3 - Vr)2 +

(KM,12) [Y+y-Ya~ - Vr)2

where Val to V 114 are the voltage at the source terminal of transistors MI to M4,

respectively. S ince V 01 V 04 arc very small compured w ith the input signals and K M1 =

K .112 = Kw= K,..u, I 1o1a1 can be approximate as shown in relation (I 0.11).

( 10.11)

Relation ( I 0.11) indicates that tho power consumption has nothing to do with signal x

anJ DC b ins X for transisto rs N 1-N 4 .

The Fig. I 0.9 shows the total current with both x and y being a 100 kHz 0.2Vp-p

sinusoidal wave. The total power consumption of first multiplier structure is 34uA when

power supply is Vo.i = 1.5 V.

30n

.12u

Hll tlOn I OQ\I

Figure 10.9 Total current consumed by the circuit for structure I

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10.4.1.4. Noise Analysis

A thermal noise current power density of a MOS transistor is conventionally

modeled as relation (I 0.12) for transistor op~rating in saturation.

(I 0. 12)

and ( I 0.13) for transistor operated in linear regions respectively [71 ].

(10.13)

The total output current noise current is given by relation ( 10.14)

(10.14)

(10. 15)

The noise performance of structure I was simulated. Fig. I 0.10 shows the

equivalent input noise within range I 0 Hz to I 00 MHz, which is 1 l 4.234n V /sqrt (Hz).

·-·-- ···--·-·-·-·-·-·. ·-·-·-·-·-·-····· ·---·--·----···-· •····-------·-.' ··" ·-· '·----.... 114 ~3311

114 H~n

111 :' Un

114 ~~!h11.,..o -~-,o-o ~--1 .. -· -~-,u-... ---1-ooK--1-M fr<Q (Hz)

··· .. , \

\ i '

i \ I

l I

i !

Figure 10.10 Equivalent input noise simulation result for structure I

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10.4.1.5 Multiplication of Analog Sign9ls

Fig. I 0. 11 shows the multiplicalions of two sinuc:oidnl w:1voo with ~u~u1.ic:i I 00

KHz and 500 KHz., applied to the multiplier structure I (Fig. 10.5). Simulation results

confim1ed that the circuit carries out the multiplication of two signols.

1 10 . , ""'

~;-

Figure 10.1 I Multiplication of two sinusoidal waves using multiplier structure I

I0.4.2 Multiplier Structure II

The multiplier strucLUre, shown in Fig. 10.12, shows a low-power multiplier

reported recently (73]. The ba~ic idea in designing this low power multiplier is to fit most

transistors into linear region und PMOS devices LO operate in saturation region,

considering the focl that PMOS transistor needs less drain current with large overdrive

voltage compared with NMOS transistor. In linear region the overdrive voltage can be

biased to increase the input range.

The drain current can remain a proper value by decreasing Vos• keeping the

power dissipation at same level (73]. Fig. I 0 .12 shows a low power CMOS analog

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multiplier structure, proposed by [73), which consist of four PMOS transistors (P1-P4)

opernting in Si:ltW-atiun region and eight NMOS transistors (Nl-N4 and Ml-M4)

operating in linear region.

Considering channel length modulation effect for MOS transistor, the drain

CUITent in Saturation region is given b y re lation ( I 0. I 6 ).

In = KJ2 (V cs - V r)2 ( l -1 A.Vos) (10.16)

where K = uCox (W/L) is the Transconductance parameter, Yr the threshold

voltage of device and A. is the channel length modulation effect for device.

\-01.J

VOi \'O~

..i Pl IJ>.j X+x Y+y

\'111.-----' .___ _ _.vv~ \ 'p3 _ _ __,

~---''J>-t

~D

1...--------------~•'----------,GND

Figure 10.12 Multiplier structure II

Assuming that all the transistors in fig.10.12 arc biased to operate in proper

region, the relation for diff~rential voltage can written as (10.17) which results in the

multiplication of two signals x and y.

V o1 - V 02 oc (K,v K M/ K,.) x*y (10.17)

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10.4.2.1 lnput Range

The= required bias conditions, to obtain the input range, for multiplier structure n

can be written as relation ( I 0. 18) and (I 0.19).

for Pl - P4

forNI -N4

(10. 18)

(10.19)

The bias voltage of Ml - M4 is chosen to be V DD in order to keep V p as low as

possible, allowing Pl - P4 for larger input range.

l 0.4.2.2 Linearity Analysis

The DC transfer characteristics of (VO! - V02) versus x and y for multiplier

structure IJ wiLh X =- 0.5 1111d Y = 1.5 are ploned in Fig. I 0.13 (a) and (b). DC transfer

characteristic; shows that second multiplier structure is four-quadrant multiplier and the

multiplier is capable to accc=pl two bipolar signals as input.

\m ... ................. l111 ......... . ... .... ·· ...

~ .. ............ - 1111 p

-: 0

.....

p ~-Im

~ .-_ ....... ... . ... - .. ··

0 ::111 •• ...... -··

-411l ..... ...

...... ··

-o: .0 I

..• ·. !.1- •!::; :~.:·:~

0 .....

,,.·· ) -.o .. : ...... ·

. ..... ·· ······· -......

. ..... _ -- ........... ... ........

.. ....

··· ... .... ..... 0 I 0:

Figure 10.13 (a) The DC transfer characteristics (V01-V02) versus x for multiplier structure II

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4 111 ... · ··· .... _,.-· ... -..... . .. ..

...... .. .. .• ··... '(• -0 : ... ••. - ···· ......... ··... . .. ··· ......

8' Jn1

:..; 0

?" G ·t in

- !111 ••

..... ··· -4m

·O.:

..... --····

... ·

. ......... ...... ..· .. ......... - ... .... ::::::~_:)~~)·-·111~~=:}~'.:· :.: - ······-············-······

..... • .....

x•O 1 •· ..• -..... ... .....

• .. ·· ...

.o l 0 ~(I)

0 l o:

Figure 10.13 (b) The DC transfer characteristics (VOI-V02) versus y for multiplier structure Tl

The linearity error of second multiplier structure fur both .y and x inputs are

shown in Fig.10.14 (a) and (b). In particular, when x = 0.12 and y = 0.2V, the linearity

error is 1.62 %. And for y = 0.12 and x = 0.2 V, the linearity error is 1.1 %.

Linearity Error

1 2

---------- -- -~-

.//

/~ _,,

~ 'c:' 0.8

~ ~ 0.0 ·c:

"' ~ 0 .4 .:J

02

0 0 04 0.06 u 12 0.16

x• 0.2V Y(V)

Figure 10.14(a) Linearity error versus y for multiplier structure II

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1 B

1 6 -- .- ~,

~ 14 / · .....,,__

~ 12 /

---. ~ 1 _ _,,/' ~OB ~ 0 6 = 0 4

02

0 0 .04 0 08 0 12 0 16

y= 0 2V x(V)

Figure I0.14(b) Linearity Error versus x for multiplier structure ll

7.~ T"'""---------------------, ~~4 +----------------------~ ------i.:-3 r-------------=- :C::::-------l

~ ~- +---------.--=--~-------'--------------1 - -'- .,,.,.,, g - 7• _,,.,,,

~ I - 'f-----~--,,7"""----------------~ -, +----..,::....-----------------~

•.is +------.----------------...!

..,~ '•'

Figure 10.15 (a) THD of output signal with x = 0.2 V for multiplier structure II

44) !> 4 ~

~ ;9~ o~

~

4 ;s! c 0 03 :J: 4 ~7 5 I-

Oi

......__ .....__

------- ..........,__ -- ---.._

n~~

o~ 4 ?.~ ! - .

~ .... : . "

Figure 10. IS(b) THD of output signal with y = 0.2 V for multiplier structure II

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The Total Harmonic Distortion {THO) is calculated when a constant DC. voltage

is applied to x (or y) while a 100 KHz 0.2Vp-p sinusoidal wave is applied toy (or x) is

shown in Fig. I 0.15 (a) and (b). The structure hus good linearity with respect to x input.

10.4.2.3 Power Consumption

The total supply current for multiplier stnicturc II, i.e. I1o11 = lri + IP2 HrJ+IP4,

is given by relation ( 10.20).

I101a1,..,, KPl/2 (Vno-X-x-Vr)2 [ l+'A (YrJll-VPJ)] + Kn/2 (VDrrX+x-Vr)2 [ l+A. (VDl)'.Vn)]

~ KrJl2 (VnrrX-x-Vr)2 [ 11-f,(Vov-VpJ)] + Kpi2 (Voo-X-lx-Vr)2 r l+l..(Voo-VN)J

(10.20)

Since V Pl - V ,,, arc very small compared with input signals (if circuit is properly biased),

the relation wi II be approximated as (I 0.21 ).

1,.,.., oc 2Kr [(V vu- X-Vr)2 + x1] (10.21)

This indicates that the power consumption has nothing to do with signal y and DC

bias Y for transistor N 1- N4. The Fig. I 0.16 shows the totaJ supply current with both x

and y being a 100 kHz 0.2Vp-p sinusoidal wave. The circuits exhibit lower consumptions

as compared to multiplier structure I. The total power consurnplion of the circuit of

multiplier structure II is 28uA, which is less as compared to that of multiplier structure I.

Figure 10.16 Total current consumed by the circuit of multiplier structure II

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l 0.4.2.4 Noise Analysis

The total output no ise for multiplier structure 11, shown in Fin. I 0.12. is given by

relation set (10.22).

(10.22)

This suggests that KM, K N and K p should be well defined lo improve the noise

performuncc. Also, the input noise depends on gm and gds that vary with the value of (X-

Y). Pig. 10.17 shows the equivalent input-referred noise integratt:d within I 0 Hz to I 00

MHz. The equivalent input noise of second multiplier structure is 867n V/sqrt (Hz).

on.

"""" -... ~ .. -·· ......... .

"""" e•~n

~

t 029n

oien ;, - ......

709n

79t>n

770<1

70lln 19 -

\ \

\

\ \,

•• frftq ( H1) '"" , ...

Figure 10.17 Equivalent input noise for multiplier structure II

10.4.2.5 Multiplication of Analog Signals

Fig. I 0.18 shows the multiplications of two sinusoidal signals, applied to the

multiplier circuit of structure II with frequencies 100 kHz and 500 KHz. The simulation

result confirms that the circuit carries out the multiplication of two signals.

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~:~~~~ ~:~­~ ~~!JfliDAMM1

e 0(1 2e.0u .. , ,...., $11.li'\I 80 e~ '~" ~ .... (.)

Figure 10.18 Multiplication of two sinusoidal signals by multiplier structure lJ

I 0.4.3 Proposed OTA Multiplier

The simplified schematic diugmm of proposed OTA multiplier, based on two

cross-coupled differential MOS pair, biased by current 21 and is shown in Fig.10.19.

Transistor Ml - M4 having same (W/L) ratio, Y+y is one input and X+x is second input

of Cross-Couple OTA multiplier, and bias current 21 can be obtained sing programmable

current source.

Vdd Proy Cun em Source

\"•

• - Y-y

.--~~~~--t~~1

M1

~r~ x+x ...

l I,

Figure 10.19 Proposed OTA Multiplier Structure

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10.4.3.I Theoretical Analysis

OT A is a Voltage Controlled Current Source (VCCS) device and hence the output

of OTA multiplier structure shown in Fig. I 0. 19 b lout= 101 - 102. Also lo1 = IoM 1 + IoM 4

and 10 2 :: loM 2 + IoM 3. Therefore Io1and 102 can be written as relation (I 0.23) and (I 0.24).

101 ~ K (Vp VT1')2 + K ( Vo-Y·VTP)2 = K (VPT)2 + K (VoT- Y)2

Im= K (VQ- V rP)2 + K (Vp-Y-V rp)2 = K (Vor)2 -r K (VPT- Y )2

(10.23)

(10.24)

where Vp and VQ arc the gntc to source voltages of M l and M2 respc~tively, K - 0.5

uCox (W /L). The I"'n current is given as lout =- 101 + 102

10111= 2K (Y+y) (X+x) (10.25)

The output equation ( I 0.25) p1ovt:s that above OTA structure can be used as fou r-

quadrant multiplier.

10.4.3.2 Linearity Analysis

The DC transfer characteristics of lout versus X and Y arc shown in Fig. I 0.20 (a)

and (b). A DC transfer characteristic shows that multiplier has four-quadrant response .

. . i • . ... -·

·-"' -· .....

o:

Figure 10.20 (a) DC characteristics: 10 • 1 versus Y (proposed multiplier)

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611

~II f'--..., ~:: f ~ -......... . :11 - · ...... ~

;: . ~ Ill I . :;. l°' I flt-ctl. i

:~:: lj . : . . ~ . -·4u \•OJ

'"'hi

.,II

-No·04--0T--.o·:~···-:oi--··6· -·-~t-·.,;r- ... 0.1-0'1

l • ·H

Figure 10.20 (b) DC characteristics: 10• 1 versus X {proposed multiplier)

The linearity error of proposed OT A multiplier with respect to inputs X and Y an:

shown in Fig. l 0.2 1 (a) and (b). In particular, when Y ::::: 0.2 and X = 0. 15, the linearity

error is measured to be 1.5 %, which is very Jess as compared to multiplier stn1ctw-cs I

und II.

Figure 10.21 (a) Linearity Error versus X ,proposed multiplier)

o~~------------------11 l 04 +---------~=--------

~ ./

! 03+-~~~~~~--~-~?~~~~~~ f 02 +-~---,,...::.~~~~~~~~-l 0 1 4------- ·- ------- -­-'

0.0~ 0 I 0.2 0.2!

YiV)

Figurel0.21 (b) Linearity Error versus Y (proposed multiplier)

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The Total Harmonic Distortion (THD) when a constant DC voltage is applied to x

(or y) and a I 00 KHz 0.2Vp-p sinusoidal wave is applied to y (or x) is shown in

Fig. I 0.22 (a) and (b). The structure of proposed OTA multiplier has good linearity with

respect to Y input. The value ofTHD increase as the input X incn:msed.

0 10

0 14

() 12

~ 0.1 ~ 008 ... 0 00

0 .0q

0 02 0

-

0 1

THO

() :

x (V)

/ /

//

/

-------

Figure 10.22 (a) THD of signnl x (proposed multiplier)

THD

o. ~ ...-------------------, 0(5 t--.~====:=;:===-----------1 04 +---------------__;~----=-----------::..-----1 o~ +------------=-...-._::;-----;;,_ __ -;

~ 0.3 +-------------------; b' 0 l!i

~ 0 .2 +---------------- ---; 01~+------------------~ 01 +---------- ---------; o~ +------------------~

O +-----.----r----..----.----~

0.0~ 0.1 0 ~. 0'

YM

Figure 10.22 (b) THD of signal y (proposed multiplier)

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10.4.3.3 Power Consumption

For constant power supply, the power consumption can be estimated by

calculating the total current. In case of OT A multiplier structure the current consumption

is almost the bias current provided by the current source, i.e. 42uA.

10.4.3.4 Simulation of Noise Performance

Fig. 10.24 shows the equivalent input-referred noise from 10 Hz to 100 MHz. The

equivalent input noise of proposed OTA multiplier structure is 11 J7 uV/sqrt (Hz), that is

slightly high as compared to previous two multiplier structures.

11.J/81.11· E.Ql.t"""~~ 11 .. UHh.•

11.J50u

11.J'4A1.1

it1..1JQ1u

~ $1t.J2ltJ >"

, , .)10\J

11.Jellu

11 ?99u

11.288u - .... . ....._......... • •• • , ._ ..... 1e 109 1t<

Noin Rnponst

- - -._

. . . . ···;flt< • ' , ....._ .. ,.00K• ' • ••••• ,..M ~-. '' "10+,, • - . "" 'l00u froq ( Hi )

Figure 10.24 Equivalent input noise (proposed multiplier)

10.4.3.5 Multiplication of Analog Signals

foig. l 0.25 shows the multiplications of two sinusoidal signals, one of frequency of

100 kHz and amplitude of 0.2Yp-p and another with frequency of 500 KHz and

amplitude of 0.2Vp-p. As a result it was confirmed that the proposed circuit carries out

the multiplication of two signals.

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In proposed OT A multiplier y input had considered n.c: n quodrntic input so it

::1hould required some biasing voltage in order to keep transistor M3 and M4 in saturation

region, while performing multiplication of two sinusoidal waves. That's why a 0.2V de

and 100 KI I~. 0.2 Vp-p sine wuvc is applie<l us other input where 0.2V de is biasing

voltage.

s:~ ~WrlrlV±dtMffl·M~~rl~ , ~:: rinAAMA~A/\;

l.~&

' · ''~ 2 1.65

1.6<' .............._~~ ............... ~ ... • 1.7:> IV•

1.5!> 0 ~011 ~ 011 6011 8011 lOOl1

1111\C(~l

Figure 10.25 Multiplication of two sinusoidal signals (proposed multiplier)

10.5 Comparison of Three Multipliers

The comparative study of three multipliers wi th n:spccl lO <lilicrcnl pcrfonnuncc

metrics is given in Table l 0.1 w1d it shows that the proposed OT A multiplier structure

has good pcrfonnnncc in tcnn of input range, linearity and power consumption but more

input noise, as compared to multiplier structures 1 and 11. The total supply current can be

further reduced by some design considerations in order to achieve less power

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consumption. The input noise can be further improved by optimizing the de value of y

and gm or transistors.

Table 10.1 Comparison of three multipliers (Vdd=3.3V)

- -Performance First Multiplier Second Multiplier Proposed OT A

Mctrh: structure structure Multipli\:r

Linearity Error of x 4.8% 1.62% 0.4& o/., - -

Linearity Error ofy 0.87 % 1.1 % 0.18 %

THD (%) ofx 2.7 4.3 0.04 -THD (%) ofy 8.6 7.3 0.388

Input Noise ll4.134n

(v/sqrt(f-12)) 867n I I .37u

Current 34uA 28uA 42uA

Consumption -~

The most important point is that OT A multiplier can be designed in two extreme

cases as for low-power (power minimization) or for low THO (THD minimization). Each

one will lead to a separate design.

163