Ultra Low Power High Speed Comparator for Analog to Digital Converters

DOI : 10.17577/IJERTV3IS110012

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Ultra Low Power High Speed Comparator for Analog to Digital Converters

Suman Biswas Department Of Electronics Kiit University Bhubaneswar,Odisha

Dr. J. K DAS

Rajendra Prasad

Abstract –Dynamic comparators with high speed , low power and low offset voltage are the main prerequisite features of all ADCs .A low power high speed and low offset dynamic comparator is being introduced in this paper. In all ADC converter architecture the basic building block is a latched comparator. The circuits are simulated in Cadence® Virtuoso Analog Design Environment in GPDK 180nm and 45nm technology. A comparison of the previous architecture and proposed comparator is shown in 180nm. The power consumption of the proposed architecture is 56% lesser than the previous architecture. The Circuit reduces the amount of kickback noise and the offset voltage making it favourable for the pipeline data conversion and flash applications.

Keyword – Comparator, low power, low offset, Kickback Noise.

  1. INTRODUCTION

    In today's world due to increase in demand for the portable battery powered devices, the necessity arises for dynamic latched comparators with high speed, low power consumption and full swing output. These comparators can become a part of high speed ADCs, sense amplifiers used in SRAM read/write circuitry and data receivers. The power in a circuit can be reduced by scaling down the feature sizes. Consequently the process variation and all other non-idealities become more significant as we move toward smaller feature sizes. The term accuracy for the Comparators is tightly constrained with its offset voltage. The power consumption is of keen interest in achieving overall higher performance in ADCs. The main drawback of pre-amp based static comparators is its high power consumption. To minimize this problem dynamic comparators are often used that makes a comparison once in every clock period and requires much lesser power.

    The dynamic comparators are of three types namely Resistor divider [2], Differential pair and capacitive- differential pair dynamic comparator.

    From these three basic architectures other structures are derived [3],[4].

    We choose differential dynamic comparator for a thorough analysis in this paper [1]. We propose new differential dynamic comparator architecture comprised of two stages namely preamplifier stage and a cross coupled latch stage.

    This paper is organized as follows: in section II analysis of conventions dynamic comparator, section III presents the

    proposed comparator architecture, section IV gives the analysis of proposed design, section V shows simulation results and section VI concludes this paper.

  2. DYNAMIC COMPARATOR DESIGN

    A. Differential pair comparator

    Fig.1 shows a pre-amplifier based dynamic comparator circuit [1]. It consists of pre-amplifier stage and a cross coupled latch circuit.

    Fig 1. Differential dynamic comparator

    The latch circuit only triggers when the preamplifier induces a sufficiently large differential voltage at the internal node of the latch. The offset due to the mismatch of cross coupled latch kicks in as soon as the amplifier begins to operate [8]. The trip point of the latch can be adjusted by sizing the input transistors [5], [6]. This dynamic comparator suffers from large kickback noise and moreover it generates a mismatch as soon as it's connected to other circuit as an input source which leads to improper operation of the Latch circuit.

  3. PROPOSED COMPARATOR

    1. Circuit architecture

      Fig.2 shows the proposed comparator architecture. It consists of two stages. The first stage is comprised of a preamplifier stage and the second stage is a latch stage. The first two stages are fed with clock Clk1 and Clk2. The mismatch effect inside the latch circuit is being overcome by separating the input transistors [1]. At the first phase both Clk1 and Clk2 are high which discharges the output node to the ground. During the second phase the Clk1 goes low which turns on the transistor M7 and M8 and the current starts to flow and charges up the node capacitor till Clk2 goes low. As soon as Clk2 goes low transistor M12

      and M13 goes off which cuts the path from the input to the cross coupled latch. This separation helps to fight back the kickback noise which is generated at the latch during decision phase. The voltage difference between the input branches and the reference differential voltage gives rise to the current Iin+ and Iin- . This process takes place during the amplification phase. During the third phase the

      Fig 2:-schematic of the Proposed Comparator

      Differential voltage is boosted in the regenerative loop of the cross coupled inverter.

      Fig. 3. Output waveform showing the swing of the proposed comparator

    2. Sensitivity analysis

    The offset of a comparator depends on different variables for that sensitivity analysis is required. The main variables for a comparator are transistors length, width, threshold voltage, carrier mobility, input and reference voltage clock signal and different parasitic capacitances. Robustness is defined by the small sensitivity to these variables. The comparator offset will be zero if the comparator is symmetric with respect to all idealities.

    Sensitivity of the comparator is defined as S Vox V /X

    x = os

    B. Time variant modelling of transistor

    During the power analysis of a dynamic comparator, the time variant model is used which emulates the operation of the transistor during dynamic operation. Existing model of MOSFET based on the separate expression for each operating region often suffers from inaccuracies near the boundaries between such regions. A single expression for drain current present in [7] is valid for all region of operation. The expression is given as follows

    id=i z[ln2(1+eVp-Vsb/2t) -ln2((1+eVp-Vdb/2t)]

    t is the thermal voltage and Vp is the pinch off voltage. This model shows a good accuracy for low voltage operation in all regions.

  4. ANALYSIS

    A. Decision point

    A comparator compares the input differential voltage with reference differential voltage Vrefdiff. The output nodes Vout+ and Vout- are discharged to the ground at the beginning. The amplification starts as soon as the clock Clk1 goes low and Clk2 still remains high. The current charges the output capacitor CL so the output rises linearly over time. The transistors M7 and M8 operate in linear region which acts as a resistor to the input transistor M5 and M6. At the beginning of the third phase the initial voltage at the output nodes are Vout+ = Iin+tamp/cL , Vout-=Iin-tamp/cL. Once the comparator enters into the third phase the sign of the Vout+ and Vout- determines which way the comparator swings. The input currents are controlled by Vin+-Vref+ and Vin–Vref- . Power is drawn only when the circuit is latched. The body terminals are shorted to their immediate sources to avoid body effect.

    [4]; where X is the amount of imbalance in the variable and where Vos is the offset voltage.

    1. Kickback noise

      The output voltage variation in CMOS latched comparators can spoil the input voltage as it is coupled to the input transistor in the circuit shown in Fig 1.The use of transistors M3 and M4 in the proposed circuit helps in the reduction of the kickback noise to further extent [9].

    2. Delay

      The delay shown in Fig. 4 can be defined as the time difference between the start of the amplification phase and the time where 50% of the final output of the latch is reached. The capacitanc value used in this architecture is less than 1fF.

      Fig. 4 delay of the comparator

    3. Power analysis

    During one period of comparison the average power of the supply voltage is obtained from the equation =fclk.Vdd. where Isupply is the current drawn from the supply voltage (Vdd) and fclk is the comparator clock frequency. During the decision making phase when Clk2=Vdd, at first both the transistor M10 & M11 both are on. As time passes, when one

    of the outputs is charged enough to turn on one of NMOS transistor (M12/M13) regeneration will commence. Assuming that the case where Vin+<Vin- , Out+ charges and eventually turns on M11 which in turn charges node Vout- to Vdd during evaluation phase. A current is drawn from Vdd from one of PMOS transistor during a short time in the dynamic operation of the decision making phase. The difference voltage in latch output(Vout+-Vout-) changes in logarithmic manner as follows Vout=Vout+-Vout-

    =Voexp(Gmt/Cload) where in this equation, Gm is the effective transconductance of the PMOS and NMOS transistors of the back to back latch inverters , Cload is the load capacitance at the comparators output and Vo is the initial voltage difference [8].The most influential design parameters on power consumption of the comparators are based upon the clock frequency, size of the input transistor

    , supply voltage and the time during which comparison is made that is the time when the peak supply current is drawn. For instance there is a trade-off in the latch inverters while deciding the sizes of PMOS transistors. Parasitic capacitances increase leads to higher power dissipation if bigger transistors are used.

    Fig.5 average power consumption of Proposed comparator

  5. SIMULATION RESULT AND COMPARISON

    The layout of the proposed comparator in 180nm technology is shown in Fig.6. The whole comparator takes an area of 185.26um2. The proposed structure in Fig. 2 is designed in Cadence 0.18u process. In table 1 key value that are being used are shown. The amplification time for the proposed comparator was set to 100ps.The proposed comparator successfully detects a difference of 1mv.

    Fig.6 layout of the proposed comparator in 180nm.

    Table 1. Key Values Used For Simulation At Same Clock Frequency

    Technology

    180nm

    45nm

    Power supply

    1.8v

    1v

    M7=M8=200/9

    M7=M8=140/3

    MOSFET size

    M5=M6=225/9

    M5=M6=40/3

    M3=M4=100/9

    M3=M4=20/3

    M1=M2=100/9

    M1=M2=8/3

    M10=M11=44/9

    M12=M13=22/9

    M12=M13=8/3

    Clock Frequency

    20G Hz

    20G Hz

    Input signal

    20M Hz

    20M Hz

    frequency

    The proposed comparator is simulated in 180nm and 45nm CMOS technologies. The power consumption of the pre- layout and post layout simulation in 180nm are shown in table 3.Comparison of the previous architecture with the proposed architecture is shown in Table 2.

    Comparators

    Offset

    Voltage(Vos)

    Power

    Delay

    Previous

    39mv

    72.95uw

    168.04ps

    architecture[1]

    Proposed

    20.98mv

    32.06uw

    160.81ps

    architecture

    Table 2.

    Fig. 7 showing the power graph of pre-layout and post layout simulation.

    Table 3.

    Pre- layout

    average power=32.06uw

    delay=160.81ps

    Post-

    layout

    average power=50.01uw

    delay=197.18ps

    The power consumption of the three sources Vdd , Vref+ and Vref- are considered as power consumption in the proposed architecture. The offset voltage calculated in this architecture is around 20.98mv.The output waveform of the proposed comparator are shown in Fig. 8.

    Fig. 8 output waveform of the proposed comparator.

    Table 4.

    Supply Voltage

    Technology 180nm

    Power Dissipation

    Delay

    1.8v

    32.06uw

    160.81ps

    1.6v

    23.92uw

    182.65ps

    1.4v

    18.97uw

    218.38ps

    1.2v

    15.63uw

    288.30ps

    Supply Voltage

    Technology 45nm

    Power Dissipation

    Delay

    1v

    1.023uw

    72.08ps

    0.9v

    0.796uw

    406.5ps

    0.8v

    0.644uw

    405.35ps

    0.7v

    0.508uw

    265.80ps

    From Table 4 it can be concluded that the comparator can work at a minimum supply voltage of 1.2v at 180nm process. Table 5 shows the variation of the power depending upon the input signal frequency. Fig. 9 shows the graph between power dissipation and the load capacitance from which it can be concluded that with the increase of the load capacitances the power dissipation increases and also at the same time the delay is increased. Table 5.a and 5.d gives the power dissipation verses input frequency in two different technologies.

    Table 5.

    Input frequency

    180nm technology

    Power dissipation

    20M HZ

    32.06uW

    40M HZ

    32.14uW

    60M HZ

    32.08uW

    80M HZ

    32.07uW

    100M HZ

    32.28uW

    Input frequency

    45nm technology

    Power dissipation

    5M HZ

    1.031uW

    10M HZ

    1.024uW

    50M HZ

    1.009uW

    100M HZ

    0.995uW

    150M HZ

    0.985uW

    Fig. 9 Power dissipation vs capacitance curve in 180nm

  6. CONCLUSION

A new dynamic comparator with low power, high speed and low offset voltage has been proposed. The power dissipation of the comparator was calculated varying the supply voltage and the input frequency. The proposed comparator was simulated in 180nm and 45nm CMOS process and their results are shown in various table. The power consumption of the proposed comparator was 56% less than the previous architecture and the speed has been increased with further reduction of kickback noise and offset voltage. A post amplifier can be connected at the output when a full swing is required.

ACKNOWLEDGEMENT

The authors would like to express their thanks to our colleagues for support in the design tool. They would also like to thank other faculties of KIIT University Bhubaneswar for assistance on various parts of this work.

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