Low Power, Low Noise Chopper Ampli er for EEG Acquisition€¦ · scribes the architecture of the...

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IEEE JOURNAL OF SOLID STATE CIRCUITS, VOL. 46, NO. 6, April 2009 1217 Low Power, Low Noise Chopper Amplifier for EEG Acquisition S. Devarakond, B. Narayan, H. Sane, J. Zaveri Abstract—This paper describes a micropower chopper stabilized amplifier for sensing EEG signals. The 4-channel EEG system utilizes a chopper stabilized amplifier and dig- ital acquisition system. The system consists of an analog multiplexer, modulator, chopper stabilized amplifier, de- modulator, level shifter and SAR ADC implemented in 0.5μm CMOS technology. The above technique provides an innovate method for eliminating the low frequency noise of the system and efficient data acquisition of the Electroen- cephanogram (EEG) signals.The input refered noise of the chopper stabilized amplifier is 52.5 nV/ Hz. The entire system consumes 850μW of power with a supply voltage of +/-3.3V. The area occupied by the system is 0.75 mm 2 . The system output consists of 10 bits in sign magnitude format. Index Terms—EEG, biopotential acquisition, flicker noise, chopper stabilization, SAR, ADC I. Introduction T HE demand for technologies that help neuroscientists and clinicians to actively observe a large number of neurons in the brain has increased significantly. Currently the biopotential acquisition systems are bulky and not portable that makes it difficult for the on-going diagnos- tics and causes discomfort to the patient. There is a need to make these systems more compact and to extend their applications to various fields. Commonly monitored biopotential signals are EEG, ECG, and EMG. Figure 1 shows the characteristics of these signals, and it can be seen that they have a very low signal amplitude and operate at extremely low frequencies (<150 Hz). This is a major reason their performance is limited by the offset and the noise of the input amplifiers. The physical origin of low frequency noise in MOSFETs can be defined from the carrier number fluctuation theory, or the trapping-detrapping model. It is caused by the fluctuation of the number of inversion layer carriers as they are trapped and detrapped to and from traps located in the oxide, and it accounts for the carrier number and the mobility fluctu- ations [1]. It should also be noted that the typical offset voltages for these applications is around 10 μV. Due to this low frequency and μV level amplitude of these signals, they are often dominated by noise. Also present are the common-mode interferences from the mains, as well as the electrode offset. Some techniques that can be employed to remove the offset and the 1/f noise dynamically include chopper sta- bilization, autozeroing (AZ), and correlated double sam- pling (CDS). While the latter two mentioned are sampling techniques, chopper stabilization is a modulation technique that can eliminate the effects of op-amp imperfections. The chopper stabilization technique was first introduced in 1948 by E.A. Goldberg [2]. Earlier, the chopping tech- Fig. 1. Frequency and Amplitude of Biopotential Signals [4]. niques involved switched ac coupling of the input signal and demodulation of this signal back to the dc signal. While these amplifiers achieved very low offset, and very high gain, they had limited bandwidth and required filter- ing to remove the large ripple voltages generated by chop- ping. This problem was solved by introducing the chopper stabilized amplifiers that combined the chopper amplifier with a conventional wideband amplifier that remained in the signal path [3]. The chopper stabilization technique essentially uses an ac carrier to perform amplitude modulation on the in- put signal. A chopper stabilized amplifier system consists of modulating and demodulating carriers with period T= 1/f chop , where f chop is the chopper frequency. It should be noted that the signal is bandlimited to half of the chop- per frequency to prevent aliasing. Figure 2 displays the relationship between noise and frequency. As seen, the 1/f noise is dominant at low frequencies, and thus the low amplitude EEG signals are susceptible to noise from the CMOS transistors. Basically, amplitude modulation using Fig. 2. Noise versus frequency [1]. a carrier transposes the signal to higher frequencies where there is no 1/f noise, and then the modulated signal is demodulated back to the baseband after amplification. A low pass filter with a cut off frequency slightly above the input signal bandwidth (>f chop /2) is used to recover the original signal in the amplified form. Noise and offset are modulated only once, and from the Power Spectral Density Equation, it can be seen that they will be translated to the

Transcript of Low Power, Low Noise Chopper Ampli er for EEG Acquisition€¦ · scribes the architecture of the...

Page 1: Low Power, Low Noise Chopper Ampli er for EEG Acquisition€¦ · scribes the architecture of the EEG acquisition system. Section III describes the analog front-end followed by Sec-tion

IEEE JOURNAL OF SOLID STATE CIRCUITS, VOL. 46, NO. 6, April 2009 1217

Low Power, Low Noise Chopper Amplifier forEEG Acquisition

S. Devarakond, B. Narayan, H. Sane, J. Zaveri

Abstract—This paper describes a micropower chopperstabilized amplifier for sensing EEG signals. The 4-channelEEG system utilizes a chopper stabilized amplifier and dig-ital acquisition system. The system consists of an analogmultiplexer, modulator, chopper stabilized amplifier, de-modulator, level shifter and SAR ADC implemented in0.5µm CMOS technology. The above technique providesan innovate method for eliminating the low frequency noiseof the system and efficient data acquisition of the Electroen-cephanogram (EEG) signals.The input refered noise of the

chopper stabilized amplifier is 52.5 nV/√Hz. The entire

system consumes 850µW of power with a supply voltage of+/-3.3V. The area occupied by the system is 0.75 mm2. Thesystem output consists of 10 bits in sign magnitude format.

Index Terms—EEG, biopotential acquisition, flicker noise,chopper stabilization, SAR, ADC

I. Introduction

THE demand for technologies that help neuroscientistsand clinicians to actively observe a large number of

neurons in the brain has increased significantly. Currentlythe biopotential acquisition systems are bulky and notportable that makes it difficult for the on-going diagnos-tics and causes discomfort to the patient. There is a needto make these systems more compact and to extend theirapplications to various fields.

Commonly monitored biopotential signals are EEG,ECG, and EMG. Figure 1 shows the characteristics of thesesignals, and it can be seen that they have a very low signalamplitude and operate at extremely low frequencies (<150Hz). This is a major reason their performance is limitedby the offset and the noise of the input amplifiers. Thephysical origin of low frequency noise in MOSFETs can bedefined from the carrier number fluctuation theory, or thetrapping-detrapping model. It is caused by the fluctuationof the number of inversion layer carriers as they are trappedand detrapped to and from traps located in the oxide, andit accounts for the carrier number and the mobility fluctu-ations [1]. It should also be noted that the typical offsetvoltages for these applications is around 10 µV. Due tothis low frequency and µV level amplitude of these signals,they are often dominated by noise. Also present are thecommon-mode interferences from the mains, as well as theelectrode offset.

Some techniques that can be employed to remove theoffset and the 1/f noise dynamically include chopper sta-bilization, autozeroing (AZ), and correlated double sam-pling (CDS). While the latter two mentioned are samplingtechniques, chopper stabilization is a modulation techniquethat can eliminate the effects of op-amp imperfections.The chopper stabilization technique was first introducedin 1948 by E.A. Goldberg [2]. Earlier, the chopping tech-

Fig. 1. Frequency and Amplitude of Biopotential Signals [4].

niques involved switched ac coupling of the input signaland demodulation of this signal back to the dc signal.While these amplifiers achieved very low offset, and veryhigh gain, they had limited bandwidth and required filter-ing to remove the large ripple voltages generated by chop-ping. This problem was solved by introducing the chopperstabilized amplifiers that combined the chopper amplifierwith a conventional wideband amplifier that remained inthe signal path [3].

The chopper stabilization technique essentially uses anac carrier to perform amplitude modulation on the in-put signal. A chopper stabilized amplifier system consistsof modulating and demodulating carriers with period T=1/fchop, where fchop is the chopper frequency. It should benoted that the signal is bandlimited to half of the chop-per frequency to prevent aliasing. Figure 2 displays therelationship between noise and frequency. As seen, the1/f noise is dominant at low frequencies, and thus the lowamplitude EEG signals are susceptible to noise from theCMOS transistors. Basically, amplitude modulation using

Fig. 2. Noise versus frequency [1].

a carrier transposes the signal to higher frequencies wherethere is no 1/f noise, and then the modulated signal isdemodulated back to the baseband after amplification. Alow pass filter with a cut off frequency slightly above theinput signal bandwidth (>fchop/2) is used to recover theoriginal signal in the amplified form. Noise and offset aremodulated only once, and from the Power Spectral DensityEquation, it can be seen that they will be translated to the

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1218 IEEE JOURNAL OF SOLID STATE CIRCUITS, VOL. 46, NO. 6, April 2009

odd harmonic frequencies of the modulating signal, leavingthe chopper amplifier without any offset or low-frequencynoise [4].

Therefore, designing the analog front-end is extremelycrucial for these applications. In order to achieve the bestsignal extraction, a front-end with high CMRR, low-noise,and high-pass filter characteristics is required, with config-urable gain and filter considerations. Hence this work de-scribes a complete EEG acquisition ASIC with low powerdissipation. This paper introduces a novel method by hav-ing a fully differential chopper stabilized micro power op-erational amplifier designed with a negative feedback thatbehaves like an inherent low pass filter, followed by a fullydifferential 10-bit successive approximation register ADC.The structure of the paper is as follows. Section II de-scribes the architecture of the EEG acquisition system.Section III describes the analog front-end followed by Sec-tion IV that describes the digital end. Section V thendescribes the various testing techniques and presents cir-cuit simulation results after system integration. The lastsection then provides the conclusion and areas for improve-ment.

II. EEG Acquisition ASIC

The figure below shows the architecture of the ASIC. Itconsists of four readout front-end channels, a bias circuit,a 10-bit SAR ADC, an analog multiplexer. Each readoutchannel is selected by an external clock, and fed to thechopper stabilized amplifier. The chopper amplifier worksat an fchop of 4 kHz. The capacitive loads are used as anegative feedback that actually behave like a low pass fil-ter. The ASIC uses a 30 kHz external clock input fromwhich the timing signals are generated by the on-chip dig-ital control circuit. A 10-bit ADC is used to digitize theoutput from the amplifier. The bias circuit is built us-ing the bandgap reference circuit topology. The ASIC hasbeen implemented in 0.5µm CMOS process.

Fig. 3. Block diagram of the EEG Acquisition ASIC

III. Analog Front End

Since EEG signals operate at very low µV ranges, thesesignals are susceptible to large amounts of common-modeinterferences, and thus a low-noise and high-CMRR ampli-fier is necessary for which chopping is commonly used. Theanalog front-end components include analog multiplexer,chopper modulator and demodulator, differential amplifierwith CMFB circuit, level shifters and bandgap referencecircuit.

A. Analog Multiplexer

The advantage of an analog multiplexer is that is allowsthe use of a single amplifier to service multiple recordingsites. The architecture used for the analog multiplexeris shown in figure 4. The input channels are Electrode1- Electrode 4. The multiplexer consists of transmissiongates that basically pass the signals when their respectiveclocks are triggered and are high impedance when the gatesare turned off. Transmission gates were chosen to preventcharge injection and clock-feedthrough. The nmos transis-tors are 15/1.05 µm, and the pmos transistors are 30/1.05µm.

Fig. 4. Schematic of the multiplexer

B. Chopper Stabilized Amplifier

The basic requirements for the amplifier were low noise,low power, high CMRR, and a considerable gain.

A fully differential micro power amplifier was designedand implemented. The input signal from the multiplexerand a reference signal of known behavior act as inputsto the chopper modulator. The architecture used for thechopper modulator is shown in figure 5. Transmission gateswere used again to avoid clock feed through issues. Thechopping frequency used was 4 kHz. Typical values used inliterature are in the range of 1 to 4 kHz. Higher frequenciescan aid in eliminating 1/f noise as much as possible. Onething to note is that due to the switching action of thetransistors, one will observe spikes in the signals. Thesespikes can be filtered using various techniques [3]. We usedthe filtering technique after demodulation to get rid of thehigh-frequency components.

Fig. 5. Schematic of the Chopper.

Once these signals are up-converted to a higher fre-quency, they are fed to the inputs of the fully differentialmicro power operational amplifier. The architecture imple-mented is shown in figure 6. The common-mode feedbackcircuit used is shown in figure 7.

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S. Devarakond, B. Narayan, H. Sane, J. Zaveri: LOW POWER, LOW NOISE CHOPPER AMPLIFIER FOR EEG ACQUISITION 1219

Adaptive biasing can reduce power dissipation in anamplifier while at the same time increase the outputcurrent drive capability [5]. When the two inputs areequal, the currents in the side branches are zero andthe diff-amp DC tail current is simply Iss. If either thepositive or the negative input increases, the currentson the respective side branches increase above zero,increasing the diff-amp tail current. Therefore, themaximum output current is limited to either Iss + Iss1or Iss + Iss2. Power dissipation can be significantlyreduced using this technique, and slew rate characteristicscan be improved greatly. Therefore, the current is given by

Iss + A((Iss1 - Iss2))

where A is the parameter that determines the gain ofthe amplifier.

These fully differential signals are then sent to the inputsof the demodulator which also has an fchop of 4 kHz.

Fig. 6. Schematic of the fully differential amplifier.

Fig. 7. Schematic of the common-mode feedback for the amplifier.

The table below lists the the specifications of the ampli-fier.

TABLE I

Amplifier transistor specifications: Active Components

Transistor ( W/L)µm Ids,uAM0, M1 15/3 7.5M11−18 4.95/1.95 4.5M21,22,23,26,27,28 4.95/3 3.5M24,25 4.95/1.05 0.400M10,19,20,29 4.95/3 7.4Current Bias Transistor 2.1/1.05 12.5

A novel method of filtering is introduced in this paper.The chopper amplifier could give a large output resistance,and when combined with a large capacitive load, they couldact as an inbuilt low pass filter, which eliminates the needto have a stand alone GmC filter. The GmC filters typi-cally consume a large area and also dissipate large amountsof power. The technique follows that of the conventionalRC filter around an active operational amplifier through anegative feedback. The capacitors can provide the neces-sary feedback to eliminate the high frequency componentsin the signals, and produce clean signals at the end of thedemodulation. The values of the capacitor are listed in thetable below.

TABLE II

Amplifier specifications after post-layout simulations

Parameter Performance ValueCF1, CF2 14 pFCL1, CL2 5 pFGain 70 dBPhase Margin 70 degreesCMRR -200 dBPSRR -250 dBPower 169.5 µWInput referred noise 52.5 nV/

√Hz

C. Level Shifter

The SAR ADC operates best when the differential sig-nals have no DC offset. So a level shifter was implemented,the schematic of which is shown in the figure below. A sim-ple technique was used to bring down the DC levels from1.65 V to 0 V.

Fig. 8. Schematic of the Level Shifter.

D. Bias Circuit

The bias circuit implemented is the Bandgap ReferenceCircuit [4]. This circuit is based on the thermal voltageself-biasing topology, and was chosen because it provides ahigh degree of supply voltage independence. The requiredvoltage from the BGR is 1.65 V.

E. Characterization of the Amplifier

The amplifier was characterized using the four differentprocess corners, and all produced similar results. The re-sults of the characterization is provided in detail below.

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Fig. 9. Schematic of the bias circuit.

The first figure gives the amplifier gain, followed by thephase. For the given range of frequencies, the amplifieris stable with over 65 degrees of phase margin. The nexttwo plots provide the input referred noise after adding thechoppers followed by the PSRR and common mode gain(or its ability to reject common mode) of the front end.It is important to note that the input referred noise be-fore adding the choppers was almost an order of magni-tude higher (800 nV/

√Hz). The input referred noise re-

duced significantly after adding the chopper to about 57nV/

√Hz, and this value dropped further after post lay-

out simulations to 52.5 nV/√Hz. This value is very com-

parable to those reported in literature, and even can beconsidered towards the lower end.

Fig. 10. Differential gain of the chopper stabilized amplifier.

Figure 16 illustrates the chopper amplifier function. Theinput signal was 10 µV, and as seen from the image, it getsamplified, and the output signal is clean due to the filteringaction.

IV. Digital and Processing End

The EEG system utilizes an ADC for performing digitalback end processing. The ADC is designed using the fullydifferential Successive Approximation topology. Successiveapproximation (SAR) ADCs provide a feasible solution forlow-power, high resolution, accurate applications. It onlyrequires one comparator regardless of the resolution, andthere is no latency for the internal clock of an SAR ADC,

Fig. 11. Phase characteristics of the amplifier.

Fig. 12. Input referred noise of the amplifier without the chopper.

which works at all times once the conversion is initiated[11].

The major blocks involved in the architecture are thefully differential capacitive main arrays and a single re-sistive array, comparator, SAR digital logic, delay, triggerand reset blocks. The block diagram of the SAR ADC is asshown in figure 17. The SAR outputs a 10 bit (N) signeddigital code. The capacitive arrays output the 6 significantbits (M) of the digital code and the resistive array providesthe last 4 bits (N-M). A single R-DAC is utilized keeping inconsideration the power consumption of the ADC circuitry.

The charge redistribution SAR ADC utilizes the capac-itive array for Track/Hold as well as the DAC. The ADCdigitizes the analog output in 12 clock cycles. The sys-tem is provided with an external as well as the internalclock working at 30 kHz and 400 kHz respectively. Thesampled differential analog signal is provided to the com-parator which outputs the signal to the digital logic. Theabove comparison of the analog signal is made with differ-ent DC voltages.

The principle of SAR ADC is based on the bootstrap-ping principle of the capacitor. The SAR ADC is initiallyreset using a global reset signal of the system. In the resetmode both the plates of the capacitor are connected to theground. In the sample mode the top plate is connected to

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S. Devarakond, B. Narayan, H. Sane, J. Zaveri: LOW POWER, LOW NOISE CHOPPER AMPLIFIER FOR EEG ACQUISITION 1221

Fig. 13. Input referred noise of the chopper stabilized amplifier.

Fig. 14. The power supply rejection ratio of the amplifier.

ground and the bottom plates to the input voltages (bot-tom plate sampling is utilized) for all the capacitors exceptthe capacitor corresponding to the MSB which is connectedto Vref . Hence the stored charge is given as:

Qx = -Ctot (Vin/2 + Vref/2)

In the hold mode the top grounding switch is thenopened and then the bottom plates are connected toground. The redistribution mode commences when theMSB is grounded during its test, while all other capacitorsare sequentially tested by connecting them to Vref initiallyand then based on the comparator output the switches areeither connected to ground or Vref for one of the DAC ar-rays and the complementary signal is provided to the otherDAC array. The equation governing the operation is givenas:

Vx =-Vin/2 + Vref (-b9/2 + b8/22 + b7/23....)

If Vx from the positive DAC array is greater than that ofthe negative DAC array the comparator switches to 1 and0 for vice-versa. The detailed explanation of the operationis provided in [12].

Thus for a 1.65V reference obtained from the BGR, theinput voltage range is in between -1.65 and 1.65 V. In ourdigital logic, MSB, which is the sign bit is 1 for a negativedifferential input voltage and is 0 for a positive differential

Fig. 15. Common mode gain of the amplifier.

Fig. 16. Outputs from the chopper stabilized amplifier.

voltage.

A. DAC

The capactive DAC consists of a series of capacitorswhich are multiples of 2 (ranging from C to C/32 in ourcase with the largest capacitor being 4 pf ). The resis-tive binary weighted sub-DAC consists of a chain of resis-tors each of 50 k-ohm. The switches present in the mainDAC as well as the sub-DAC are transmission gates used tominimize the clock feedthrough as well as input dependentcharge injection. Since the ADC has an accuracy of 10-bit,the challenge involves in ensuring that the delay due to theresistances of the switches and the varied capacitances re-main relatively constant. This was ensured using relativesizing of the transmission gates. The test case designed forthe R-Sub DAC is shown below in figure 18.

The sampled input signal of 100 mV differential ampli-tude is digitized through charge distribution principle asshown in the next figure.

B. Comparator

The comparator consists of a pre-amplifier followed bya memoryless sense amplifier and an SR latch. The Com-parator diagram is shown in figure 20.

The comparator works on clock and clock-bar signalswhich ensure memoryless operation by pulling the nodesof the comparator to known Vdd and gnd states. Thus thedesign implemented does not have memory effects and thefinal stage of the implemented circuit consists of a latch

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1222 IEEE JOURNAL OF SOLID STATE CIRCUITS, VOL. 46, NO. 6, April 2009

Fig. 17. Block diagram of the ADC.

Fig. 18. Test bench of the resistive DAC.

which holds the current state until the next state is ob-tained. The output of the comparator test bench is asshown in figure 21 for complementary input signals.

C. SAR Digital block implementation

The digital implementation of the circuit is shown infigure 22 and is a standard implementation consisting of Dflip-flop followed by registers and SR latches. N-MOS andP-MOS switches are utilized to reset the signals.

An internal generated pulse triggers the circuit andbased on the output generated from the comparator, eachof the bit is switched.

The ADC test signal which consists of a single sinusoidaltest signal of frequency 128 Hz is used and the outputdigital code corresponding to the digital signal is shown infigure 24, figure 25. There exists a change in the frequencyof the signal due to the clock frequency not being an integermultiple of the input signal and due to variable transientnature of the cadence simulation environment.

The PSD of the ADC is calculated with 226 sampledand is shown in figure 27. Repeated averaging of the signalwould provide better ENOB and SNDR results.

The characteristics of the ADC is listed below in theTable (III).

TABLE III

ADC specifications

Parameter Performance ValuePower Consumption 700 µWSNDR 40 dBENOB 7DNL 1.5 LSB

Fig. 19. Digitized codes through charge redistribution principle.

Fig. 20. Schematic of the Comparator.

V. Integrated System

The schematic of the integrated system is shown in fig-ure 27. The comparison of this work along with othersis presented in figures 28 and 29. There were a trade-offswith respect to input referred noise and power and area,and an optimal value was selected that gave a good bal-ance of the two. The fully differential SAR was designedbased entirely on logic since there weren’t any designs dis-cussed in literature. The final system results are discussedin Appendix 1.

Figure 30 gives a picture of the pad frame. The area ofthe chip is 0.81mm2.

VI. Conclusion

A novel low power, low noise chopper stabilized ampli-fier for EEG acquisition was described. With area, power,stability, and portability as the criteria, different figures ofmerit for the analog and digital ends were obtained. Thesystem was built on 0.5µm process, and it was implementedon a 0.81mm2 chip. The system integration results werediscussed. The novel techniques introduced in this paperwere the use of micropower chopper stabilized amplifierthat effectively reduced the input referred noise by an or-der of magnitude. The low pass filtering technique wasalso new, and it helped eliminate the unwanted high fre-quency noise. The high resolution fully differential 10-bitcharge redistribution SAR ADC was also novel in its logicimplementation, and provides significant resolution duringthe analog to digital conversion.

References

[1] Y. Nemirovsky, I. Brouk, C. Kakobson, 1/f Noise in CMOS Tran-sistors for Analog Applications, IEEE Transactions on ElectronDevices vol. 48, no. 5, May 2001.

[2] R.F. Yazicioglu, et. al., A 200 µW Eight-Channel EEG Acquisi-tion ASIC for Ambulatory EEG Systems, IEEE Journal of SolidState Circuits vol. 43, no. 12, December 2008.

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S. Devarakond, B. Narayan, H. Sane, J. Zaveri: LOW POWER, LOW NOISE CHOPPER AMPLIFIER FOR EEG ACQUISITION 1223

Fig. 21. Comparator output check.

Fig. 22. Block Diagram of the SAR digital implementation.

[3] D. Yates, E. Lopez, et. al. A Low-Voltage Low-Power Front-Endfor Wearable EEG Systems, IEEE EMBS Conference Proceed-ings August 23-26, 2007.

[4] R.F. Yazicioglu, et. al., A 60µW 60 nV/rt.Hz Readout Front-Endfor Portable Biopotential Acquisition Systems, IEEE Journal ofSolid-State Circuits vol. 42, no. 5, May 2007.

[5] M. Dagtekin, W. Liu, R. Bashirullah, A Multi Channel ChopperModulated Neural Recording System, IEEE EMBS ConferenceProceedings October 25-28, 2001.

[6] J. Arias, et. al. Design of a CMOS Fully Differential Switched-Opamp for SC Circuits at very low power supply voltages, ICECSConference, Spain 2001.

[7] Y. Masui, T. Yoshida, A. Iwata Low Power and low voltagechopper amplifier without LPF , IEICE Electronics Express vol.5, no. 22, 2008.

[8] T. Denison, K. Consoer, A. Kelly et. al., A 2.2 µW 94 nV,rt. Hz, Chopper-Stabilized Instrumentation Amplifier for EEGDetection in Chronic Implants ISSCC Dig. Tech. Papers pp.162-163, 2007.

[9] A. Bakker, K. Thiele, J. Huijsing, A CMOS Nested-ChopperIntrumentation Amplifier with 100-nV Offset , IEEE Journal ofSolid State Circuits vol. 35, no. 12, December 2000.

[10] V. Mognon, et. al., Capacitive-SAR ADC Input Offset Reduc-tion by Stray Capacitance Compesation, Devices, Circuits, andSystems 2008.

[11] V. Mognon, et. al., Capacitive-SAR ADC Input Offset Reduc-tion by Stray Capacitance Compensation, Devices, Circuits, andSystems 2008.

[12] G. Promitzer, 12-bit low-power fully differential switched capac-itor noncalibrating successive approximation ADC with 1MS/s,IEEE Journal of Solid State Circuits vol. 36, no. 7, May 2001.

[13] Christian C. Enz, Gabor C. Temes, Circuit Techniques for Re-ducing the effects of Op-Amp Imperfections: Autozeroing, Cor-related Double Sampling, and Chopper Stabilization, Proceedingsof the IEEE vol. 84, no. 11, November 1996.

[14] S. Brigati, et. al., Modeling Sigma-Delta Modulator Non-Idealities in SIMULINK

VII. Appendix

A. Compairson Chart

Figure 31 gives the outputs of various stages after systemintegration.

Fig. 23. Test bench output for ADC

Fig. 24. Digital output codes of the first five bits in the ADC testbench setup.

Fig. 25. Digital output codes of the last five bits in the ADC testbench setup.

Fig. 26. PSD of the ADC.

Fig. 27. Schematic of the entire system with the Analog Front-Endand Digital and Processing End.

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1224 IEEE JOURNAL OF SOLID STATE CIRCUITS, VOL. 46, NO. 6, April 2009

Fig. 28. Input Referred Noise comparison chart.

Fig. 29. Power consumed by front-end.

Fig. 30. Padframe of the EEG Acquisition ASIC.

Fig. 31. System integration results.

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ECE 6414 Team 4: Low Power, Low Noise EEG

Acquisition System

S. Devarakond, B. Narayan, H. Sane, J. Zaveri

November 12, 2009

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Contents

1 Introduction 2

2 Padframe Details and Pictures 52.1 Pin Description . . . . . . . . . . . . . . . . . . . . . . . . . . 52.2 X-Ray Images . . . . . . . . . . . . . . . . . . . . . . . . . . . 6

3 Observations and Measurements 103.1 Setup . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 103.2 Measurement Results . . . . . . . . . . . . . . . . . . . . . . . 11

1

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Chapter 1

Introduction

The demand for technologies that help neuroscientists and clinicians to ac-tively observe a large number of neurons in the brain has increased signif-icantly. Currently the biopotential acquisition systems are bulky and notportable that makes it difficult for the on-going diagnostics and causes dis-comfort to the patient. There is a need to make these systems more compactand to extend their applications to various fields.

Commonly monitored biopotential signals are EEG, ECG, and EMG.Figure 1 shows the characteristics of these signals, and it can be seen thatthey have a very low signal amplitude and operate at extremely low fre-quencies (<150 Hz). This is a major reason their performance is limitedby the offset and the noise of the input amplifiers. The physical origin oflow frequency noise in MOSFETs can be defined from the carrier numberfluctuation theory, or the trapping-detrapping model. It is caused by thefluctuation of the number of inversion layer carriers as they are trapped anddetrapped to and from traps located in the oxide, and it accounts for thecarrier number and the mobility fluctuations [1]. It should also be notedthat the typical offset voltages for these applications is around 10 µV. Dueto this low frequency and µV level amplitude of these signals, they are oftendominated by noise. Also present are the common-mode interferences fromthe mains, as well as the electrode offset.

Some techniques that can be employed to remove the offset and the1/f noise dynamically include chopper stabilization, autozeroing (AZ), andcorrelated double sampling (CDS). While the latter two mentioned are sam-pling techniques, chopper stabilization is a modulation technique that caneliminate the effects of op-amp imperfections. The chopper stabilizationtechnique was first introduced in 1948 by E.A. Goldberg [3]. Earlier, thechopping techniques involved switched ac coupling of the input signal anddemodulation of this signal back to the dc signal. While these amplifiersachieved very low offset, and very high gain, they had limited bandwidthand required filtering to remove the large ripple voltages generated by chop-

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Figure 1.1: Frequency and Amplitude of Biopotential Signals [1].

ping. This problem was solved by introducing the chopper stabilized am-plifiers that combined the chopper amplifier with a conventional widebandamplifier that remained in the signal path [4].

The chopper stabilization technique essentially uses an ac carrier to per-form amplitude modulation on the input signal. A chopper stabilized am-plifier system consists of modulating and demodulating carriers with periodT= 1/fchop, where fchop is the chopper frequency. It should be noted that thesignal is bandlimited to half of the chopper frequency to prevent aliasing.Figure 2 displays the relationship between noise and frequency. As seen, the1/f noise is dominant at low frequencies, and thus the low amplitude EEGsignals are susceptible to noise from the CMOS transistors. Basically, ampli-

Figure 1.2: Noise versus frequency [2].

tude modulation using a carrier transposes the signal to higher frequencieswhere there is no 1/f noise, and then the modulated signal is demodulated

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back to the baseband after amplification. A low pass filter with a cut offfrequency slightly above the input signal bandwidth (>fchop/2) is used torecover the original signal in the amplified form. Noise and offset are mod-ulated only once, and from the Power Spectral Density Equation, it canbe seen that they will be translated to the odd harmonic frequencies ofthe modulating signal, leaving the chopper amplifier without any offset orlow-frequency noise [4].

Therefore, designing the analog front-end is extremely crucial for theseapplications. In order to achieve the best signal extraction, a front-endwith high CMRR, low-noise, and high-pass filter characteristics is required,with configurable gain and filter considerations. Hence this work describesa complete EEG acquisition ASIC with low power dissipation. This paperintroduces a novel method by having a fully differential chopper stabilizedmicro power operational amplifier designed with a negative feedback thatbehaves like an inherent low pass filter, followed by a fully differential 10-bit successive approximation register ADC. The structure of the paper isas follows. Section II details the padframe and the pin assignments. Sec-tion III gives an overview of the test-setup and measurement results andobservations.

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Chapter 2

Padframe Details andPictures

2.1 Pin Description

The figure below gives the pin description for the chip.

Pin Description Pin Description1 Padnc 21 Vim

2 Padnc 22 Vip

3 Padnc 23 phi14 Ground 24 Reset Global5 Digital Vdd 25 ExtClk6 Padnc 26 Bit97 -Vdd 27 Bit88 Clk3 28 Bit79 Clk2 29 Bit610 Clk1 30 Bit511 Clk0 31 Bit412 I0 32 Bit313 I1 33 Bit214 I2 34 Bit115 I3 35 Bit016 I4 36 Padnc17 Vref 37 Padnc18 Vdd 38 Padnc19 Clk Chopper 39 Padnc20 Clkbar Chopper 40 Padnc

The final padframe image is shown in figure 2.2.

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Figure 2.1: Pin Description.

Figure 2.2: EEG ASIC Padframe.

2.2 X-Ray Images

A few X-ray images were taken to verify the wire-bonding on the chip,before we started the testing. The following figures illustrate the X-ray

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image results. There were no wire-bonding issues observed.

Figure 2.3: X-Ray Image 1.

Figure 2.4: X-Ray Image 2.

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Figure 2.5: X-Ray Image 3.

Figure 2.6: X-Ray Image 4.

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Figure 2.7: X-Ray Image 5.

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Chapter 3

Observations andMeasurements

3.1 Setup

The chip was tested after tapeout. The figure (3.1) below shows the testmeasurement setup. We implemented a detailed setup process, as follows: 1)Testing the Power Supplies and Ground Connections 2) Testing the Outputfrom the Bandgap Reference Circuit 3) Testing the Output from the AnalogFront-End 4) Testing the Output pins of the ADC

In the figure below, it is seen that the chip was placed on a protoboard,to avoid any soldering issues. This chip was solely used to test the powersupply and ground connections.

Figure 3.1: Test Setup.

Figure 3.2 shows the entire setup, along with the function generators,

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DMM, and oscilloscope. For each connection, we observed the current drawnfrom the supply, and the output in the oscilloscope. For the first stage, weonly tested the supplies and the analog front-end.

Figure 3.2: Detailed Test Setup.

3.2 Measurement Results

It was observed that once the analog Vdd and ground pins were connectedusing the power supply, the current drawn was in the order of mA. Thisdoes not match the simulated results, where the total current did not exceed120 µA. Once the analog Vdd and ground were connected, we observed thefollowing:

Pin Description Voltage (V)5 Vdd 3.37 -Vdd 3.38 Clk3 09 Clk2 010 Clk1 011 Clk0 012 I0 013 I1 014 I2 015 I3 021 Vim 2.23122 Vip 2.23823 phi1 3.3

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It was important to analyze the source of this large current. The BGRoutput was zero, and it was observed that there was an open circuit. There-fore, we forced a voltage of 1.65 V at the BGR pin, and checked the currentdrawn, and it was still in the mA range.

After further analysis of the layout, we discovered that we had shortedthe analog, and digital Vdd, as well as the plus and minus Vdd. This errorwas at the padframe level, where we connected the power supplies to thepadvdd, and hence there was a short.

This project a great learning experience, and we are grateful to ourProfessor Dr. Ghovaloo, Mehdi Kiani and MOSIS. The project gave us asound understanding of analog systems - from a chip design, layout, testingand verification standpoint. We are in the process of analyzing the chipfurther, and will report any new findings in the near future.

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Bibliography

[1] R.F. Yazicioglu, et. al., A 60µW 60 nV/rt.Hz Readout Front-End forPortable Biopotential Acquisition Systems, IEEE Journal of Solid-State Circuits vol. 42, no. 5, May 2007.

[2] Y. Nemirovsky, I. Brouk, C. Kakobson, 1/f Noise in CMOS Transis-tors for Analog Applications, IEEE Transactions on Electron Devicesvol. 48, no. 5, May 2001.

[3] R.F. Yazicioglu, et. al., A 200 µW Eight-Channel EEG AcquisitionASIC for Ambulatory EEG Systems, IEEE Journal of Solid StateCircuits vol. 43, no. 12, December 2008.

[4] D. Yates, E. Lopez, et. al. A Low-Voltage Low-Power Front-Endfor Wearable EEG Systems, IEEE EMBS Conference ProceedingsAugust 23-26, 2007.

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