Simultaneous Measurement of Nonlinearity and ...Measured Biological Data before...

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Simultaneous Measurement of Simultaneous Measurement of Nonlinearity and Electrochemical Nonlinearity and Electrochemical Impedance for Protein Sensing Using Impedance for Protein Sensing Using Two Two-Tone Excitation Tone Excitation Jon Daniels, Ph.D. Candidate [email protected] IEEE EMBC08 24-Aug-08 SuBT2.5 Stanford Department of Electrical Engineering Stanford Genome Technology Center (SGTC) Co-authors: Erik P. Anderson – Stanford EE, SGTC Prof. Thomas H. Lee – Stanford EE Prof. Nader Pourmand – SGTC, UC Santa Cruz

Transcript of Simultaneous Measurement of Nonlinearity and ...Measured Biological Data before...

Page 1: Simultaneous Measurement of Nonlinearity and ...Measured Biological Data before Jon.Daniels@stanford.edu IEEE EMBC08 24-Aug-08 SuBT2.5 13 0 50 100 150 Electrode Bias [mV] 0 50 100

Simultaneous Measurement of Simultaneous Measurement of Nonlinearity and ElectrochemicalNonlinearity and Electrochemical

Impedance for Protein Sensing Using Impedance for Protein Sensing Using TwoTwo--Tone ExcitationTone Excitation

Jon Daniels, Ph.D. [email protected]

IEEE EMBC08 24-Aug-08 SuBT2.5

Stanford Department of Electrical EngineeringStanford Genome Technology Center (SGTC)

Co-authors:

Erik P. Anderson – Stanford EE, SGTC

Prof. Thomas H. Lee – Stanford EE

Prof. Nader Pourmand – SGTC, UC Santa Cruz

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Affinity Affinity BiosensorsBiosensors

• Immobilized probe selectively captures target

• Target capture changes surface propertiesIncubation,

probe

target

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properties

• Detecting change in surface properties = detecting target

Incubation,washing

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Probe Layer

Solution

Impedance for Affinity Impedance for Affinity BiosensorsBiosensors

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• Binding changes electrical properties of surface

• Selectivity determined by probe layer => platform amenable to various applications by changing probe

Electrode

Probe Layer

(Insulator)( )

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Measuring ImpedanceMeasuring Impedance

I

+

Vout

Vin

Zf

ZDUT

Vout = -Vin (Zf /ZDUT)

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V

Vout = -Vin (Zf /ZDUT)

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Electrode “Electrode “ImpedanceImpedance” is Nonlinear” is Nonlinear

• Electrode-electrolyte impedance depends (quite strongly) on DC bias => nonlinear

• ionic double layer capacitance:

Cdl(φ) =(

228 µF/cm2)

C0

mol/L

(

1 +1

8

(

φ

VT

)2)

I

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( )

mol/L

(

8

(

VT

)

)

I

V

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Question #1Question #1

Can changes in nonlinearity be used to discriminate target binding?

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vs. ?

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Question #2Question #2

Can nonlinearity be quantified without extra measurement time?

I

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I

V

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Measuring Nonlinearity w/ 2 tonesMeasuring Nonlinearity w/ 2 tones

Vin = A cos(ωAt) + B cos(ωBt)

ZDUT (ω) = Z0(ω)(

1 + α1Vin + α2V2in

)

Vout = −Vin

Zf(ω)

Z0(ω)

1

1 + α1Vin + α2V2in

−Z (ω )

+

Vout

Vin

Zf

ZDUT

Vout = -Vin (Zf /ZDUT)

Conventional Low frequency

Small-signal impedance

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Vout =−Zf (ωA)

Z0(ωA)A cos(ωAt)

+ 12α1AB

Zf (ωA−ωB)

Z0(ωA−ωB)cos((ωA − ωB)t)

+ 12α1AB

Zf (ωA+ωB)

Z0(ωA+ωB)cos((ωA + ωB)t)

+ 14α2AB

2 Zf (ωA−2ωB)

Z0(ωA−2ωB)cos((ωA − 2ωB)t)

+ 14α2AB

2 Zf (ωA+2ωB)

Z0(ωA+2ωB)cos((ωA + 2ωB)t)

+ other terms far removed from ωA

Small-signal impedance

IM2

IM3

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ADCFFT

Select DUT

Tone Outputs

0.1-100 kHz

PC with LabViewand ADC/DAC card

chip with 36electrodes

ωΑ

System DiagramSystem Diagram

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+

ZDUT,1 16:1

ZDUT,16

Σ

17 Hz

Zf

PCB

electrodes

Vout

Vin

ωΒ

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PCB ImplementationPCB Implementation

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12.35

12.4

12.45

12.5

Cap

acit

ance

[n

F]

10 nF

1 kΩ

Validating Measurement ApproachValidating Measurement Approach

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−100 −75 −50 −25 0 25 50 75 100

12.2

12.25

12.3

12.35

Bias [mV]

Cap

acit

ance

[n

F]

o = measured manually with custom setup

= measured manually with commercial LCR meter

– = extrapolated from nonlinearity tones at 0 mV

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Making “Biology” Happen is HardMaking “Biology” Happen is Hard

fluorescently-labeledstreptavidin BSA BSA-biotin

polymer multilayer

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300µm electrodes

Contact pads

O-ring (holds solution)

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10

11

12

13

14

15

CPE Magnitude ["nF"]

0.9

0.905

0.91

0.915

0.92

0.925

CPE phase parameter

24

25

26

27

28

29

30

|Zdut

| @ 1 kHz [kΩ]

Measured Biological DataMeasured Biological Data

before

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0 50 100 150Electrode Bias [mV]

0 50 100 150Electrode Bias [mV]

0 50 100 150Electrode Bias [mV]

0 50 100 150

10

11

12

13

14

15

Electrode Bias [mV]

CPE Magnitude ["nF"]

0 50 100 150

0.9

0.905

0.91

0.915

0.92

0.925

Electrode Bias [mV]

CPE phase parameter

0 50 100 150

24

25

26

27

28

29

30

Electrode Bias [mV]

|Zdut

| @ 1 kHz [kΩ]

after addition of1 µg/mL avidin

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−0.02

0

0.02

0.04

0.06

α1 [

V−

1]

Nonlinearity Nonlinearity Indicates BindingIndicates Binding

change after addition of250 ng/mL avidin

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BSA−biotin (positive) BSA (negative)

−0.08

−0.06

−0.04

−0.02

∆ α

1

n=4 n=8

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ConclusionsConclusions

• Two-tone approach allows simultaneous measurement of small-signal impedance and nonlinearity– No extra measurement time

– Cost is redesigning measurement apparatus

• Nonlinearity can indicate target binding

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• Nonlinearity can indicate target binding

• Nonlinearity appears to be influenced by surface charge– Surrogate for field-effect sensor?

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Questions?Questions?

Suggestions?Suggestions?

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Suggestions?Suggestions?

[email protected]@stanford.edu

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Backup SlidesBackup Slides

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Backup SlidesBackup Slides

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What is Impedance?What is Impedance?

• impedance = measure of opposition to a sinusoidal alternating electric current, generalizing Ohm's law to AC circuit analysis

• impedance = ∆voltage / ∆current

Z = 1000 + 15915 j Ω10 nF

[email protected] 18IEEE EMBC08 24-Aug-08 SuBT2.5

15915 j Ω

1000 Ω

10 nF

|Z| = 15947 Ω

θZ = -86.4°

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Impedance SpectroscopyImpedance Spectroscopy

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Source: http://www.gamry.com/App_Notes/EIS_Primer/EIS_Primer.htm

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Affinity DetectionAffinity Detection

Kd =koff

kon, probe coverage

Readout/transducer type

Transducer

Selective Probe

Electrical

Chemical

Target concentration

Target surface coverage

Surface property change

affinity

readout

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Post-processing

Amplifier

Data Acquisition

Transducer

Acquired

Electrical

(a) (b) (c)

Measured change

Instrumentation

Surface property change readout

Daniels/Pourmand, Electroanalysis 19:1239-1257 (2007)

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Typical Measurement ApproachTypical Measurement Approach

$10-30k

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• Single electrode measurement

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Custom Measurement ApparatusCustom Measurement Apparatus

300µm electrodes

Contact pads

O-ring (holds solution)Rknown

Vin

DUT

Computerwith LabView

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Socket

PCB with circuitry

Chip

Vout

DUT

ZDUT = -(Vin/Vout)*Rknown

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Double Layer CapacitanceDouble Layer Capacitance

• α2 ~ 188 V-2 for double layer capacitance according to Gouy-Chapman model

• Predict α ~ 14 V-2 in our measurement based

Cdl(φ) =(

228 µF/cm2)

C0

mol/L

(

1 +1

8

(

φ

VT

)2)

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• Predict α2 ~ 14 V-2 in our measurement based on voltage across ionic layer (vs. interface)– expect less due to Stern modification

• We observe |α1| ~ 0.1-1 V-1 and |α2| ~ 1-10 V-2

in all our measurements

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Next StepsNext Steps

• Custom measurement IC design (in progress) and testing

• Explore nonlinear effects with constant phase element?

• Try “real biology”?

[email protected] 24IEEE EMBC08 24-Aug-08 SuBT2.5

• Graduate and get a “real job”!

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AcknowledgementsAcknowledgements

• Nader Pourmand, Prof. Ron Davis (Biochem)

• Erik Anderson, Prof. Tom Lee (ElecEng)

• Heng Yu (surface chemistry)

• Other SGTC personel

• NIH and NSF for direct and indirect funding

[email protected] 25IEEE EMBC08 24-Aug-08 SuBT2.5

• NIH and NSF for direct and indirect funding