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SPNSWTCH Workshop „Spin Momentum Transfer” , Kraków 2008 Low Noise Mix-Mode Integrated Circuits for Micro-sensor readout Paweł Gryboś Department of Measurement and Instrumentation AGH University of Science and Technology

Low Noise Mix-Mode Integrated Circuits for …†“NSW↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008 Low Noise Mix-Mode Integrated Circuits for Micro-sensor readout

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S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Low Noise Mix-Mode Integrated Circuits for Micro-sensor readout

Paweł GrybośDepartment of Measurement and Instrumentation

AGH University of Science and Technology

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

1. Introduction: multichannel low noise integrated circuit

2. Noise, crostalk and matching

3. Digital imaging system for diffractometry applications

4. Multichannel neurobiology experiments

5. Conclusions

Outline

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Multichannel low noise ASIC

Input signals- small amplitude (Qin = 1400 el, Vin = 50 μV)- stochastic character (amplitude, time)

SET OF SENSORS ( silicon strip detector, neuronal cells of retina)

MULTICHANNEL INTEGRATED CIRCUITS (analogue & digital blocks)

CROSSTALKdigital ⇔ analogue

LIMITS: power & area

LOW LEVELOF NOISE

UNIFORMITY OFPARAMETERS

6.5

mm

RX64 NEURO64

Microsensors50-100 μm

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Noise in MOS transistors

mth kTg

dfdi

382

=

saturation

dsth kTg

dfdi 4

2

=

linear

Simulations (HSPICE) NLEV=3 ( ) GDSNIO

aaaVV

LWCkT

dfdi

TGSoxth

+++

−=1

13

8 22

μ

BSIM3v3 (NIMOD=2) inveff

effth QL

kTdfdi

2

2 4 μ=

1. Thermal noise of channel

Measurments – short channel effects (2-10x):( velocity saturation, hot electrons)

2. Flicker noise

Simulations (HSPICE)

NLEV=2, 3 AFeffeff

m

ox

f

fLWg

CKF

dfdi 122

/1 =

Measurments – short channel effects( hot electrons, RST noise)

BSIM3v3 (NIMOD=2)

Time

V(t)

Signal Signal+noise

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

CROSSTALK

Transfer:- common supply lines: parasitic inductance i resistance (Vind=LdI/dt)- common substrate: (substrate⇒epi, VT=f(VSB), gmb)

Effects for analogue blocks: switching noise, oscillation etc.

Minimisation:- reducing the noise generation,- increasing the immunity of analogue part,- isolation techniques.

GENERATIONTRANSFER EFFECT

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

RANDOM MATCHING

( ) 222

2 DSWLAP P

P +=Δσ

For MOS transistors: VT0 , β, γ

ox

BFs

ox

oxFMST0 C

NqCQV

φεφφ

42 +−+=

LWCoxμβ =

ox

Bs

CNqε

γ2

=

CMOS 0.7μm - σ(VT0) NMOS PMOS

W/L=2μm/0.7μm 9.72 mV 19.43 mV

W/L=1500μm/1.5μm 0.31 mV 0.63 mV

L

W

L

W

D

MATCHING - identically design devices have different parameters ΔP=P1-P2 (ΔP/P)

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Two Examples of Low Noise Mix-Mode Integrated Circuits

Diffractometry Neurobiology

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Digital X-ray Imaging System

Digital Imaging System(X-rays photon counting)

Position sensitive systemwith a good spatial resolution

High dynamic range &relatively high X-ray intensity

Energy window selectionfor X-ray photons

MULTICHANNELSYSTEM

+ ARRAY OF SENSORDISCRIMINATORS

SHORT TIME OFPULSE PROCESSING

Applications:- clinical diagnostic: dual energy mammography & angiography- material science - diffractometry

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Scheme of imaging system

Silicon strip detector⇓

• good spatial resolution: tens of μm

• energy resolution: 3.67 eV/e-h

• single photon counting mode

• good efficiency

Multichannel ASIC(analog processing + data storage)

• binary readout architecture to cope with high X-ray intensity

• selection of pulses according their amplitude

control,data

X- ray

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Problems with binary readoutfor X-ray applications

Pulse height spectrum

1) Counting pulses N

2) dN/dVTH

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Multichannel ASIC architecture

DEDIX: Dual Energy Digital X-ray Imaging

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Single channel architecture (ASIC – 64 channels)

RX64:CMOS 0.8 umTp=800 ns

DEDIX :CMOS 0.35 umTp = 160 ns

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Why correction is necessary?

DC coupling between stages – base line changes from channel to channel

BaseLine

VT HIGH

VT LOW

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Spectrum of X-ray source – measurement set-up

Pu-238 source

Cu (Fe, Zn) foil

Si strip detector DEDIX

Serial output

13.6; 17.2; 20.1 keV

8.04keV

eleV

keVQ

eleV

keVQ

eleV

keVQ

eleV

keVQ

547667.31.20

468667.32.17

370567.36.13

219067.3

04.8

4

3

2

1

==

==

==

==

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Correction procedure

1. Measurement with external X-ray source gives useffective voltage spread (constant correction)

2. Measurements with internal generation circuit anddifferent correction DAC’s value gives us theirnonlinear characterisation

3. Calculation the value of correction DAC’s – we know how much we want our threshold to be moved(1) and we know what DAC’s value move thethreshold to correct value (2)

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

High count-rate measurement with X-ray tube

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

SSD in diffractometry

X-ray tube

+ detectormoving

slit

sample under test

ASIC

silicon strip detector+ DEDIX chip

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Detectors with different pitch

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Continous scan (prof. T. Stobiecki laboratory)

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Fluorescence suppression - Rigaku, Japan

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

CCD detector

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Readout of CCD

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Pixel detector Si/GaAs

Picture: CERN

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Bump Bonding

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Medipix -CERN

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Medipix -CERN

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Medipix -CERN

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Medipix -CERN

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

PILATUS - PSI

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

PILATUS- PSI

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Low Noise Mix-Mode Integrated Circuits for Neurobiology Applications

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

History – single channel recording

‘Patch-clamp’ technique : Neher & Sakmann, 1976, (Nobel Prize1991)

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Neural systems

BRAIN

RETINA

Cones: 6.5 x 106 (colours)Rods: 125 x 106 (move, shape)Optical nerve: 1 x 106 fibers

Photo: Biologia, PWN

Single neuron

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Motivation

1.Understand neuronal coding,

2. Biosensors

3. Neuronal prostheses

for recording/stimulation of neuronal system comprising several hundreds or thousands of electrodes

AIM: to build an electronic interface

Components

1.Microelectrode array

2. Multichannel electronics

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Microelectrode arrays I – planar microelectrodes

Ayanda Biosystems

Multi Channel SystemsUniversity of Glasgow

512-electrode array 32x16: spacing = 60 um diameter = 5 um

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Microelectrode arrays II - Microprobes

NeuroNexus Technologies

Utah Microelectrode Array

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Recording/stimulation electronics – standart solutions

60-channel recording system

8-channel stimulus generator

4-channel recording amplifier

Limits:

- number of channels

- large volume and weight

- high costs

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Multichannel neuribiological recording based on ASIC

MICROELECTRODES ARRAY

analogue multiplexer

control data

MULTICHANNEL ASIC COMPUTER

To design a multichannelAPPLICATION SPECIFIC INTEGRATED CIRCUIT (ASIC),

which is able to cope with extracellular neuronal recording

• to built recording system comprising several hundreds or thousands of electrodes

• miniaturization

system

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Extracellular recording – requirements for electronics

Requirements:

Low noise ~ 5 μV rms Frequency band pass 20 Hz to 2000 HzAC coupled input cut-off frequency < 20 Hz

Signal source (e.g. retina tissue): Vamp = 50-500 μV, DC offsets,tw ≈ 1-2 ms, band: 20 -2000 Hz,

MULTICHANNEL ARCHITECTURE

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Multichannel architecture

LIMITATION OF CMOS TECHNOLOGY

64 channel ASIC - NEURO64 Single channel architecture

CMOS technology 0.7 um4 mm x 6 mm

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

CMOS technology - noise

MOS transistors:- flicker noise ⇐ low frequency,- thermal noise ⇐ power limitation

AC-coupling -kT/C noise:- small capacitors ⇐ area limitationCMOS technology: C= 1pF ⇒ 64μV rms

C= 100pF ⇒ 6.4μV rmsSMD technology: C= 10nF ⇒ 0.64μV rms

Crosstalk:- supply bounce, - substrate noise

R

Creadoutelectrode

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Low noise preamplifier

fLKLK

LWCK

dfdv

fpp

fnn

ox

fpdiff 112

23

21

11

2_/1

⎟⎟⎠

⎞⎜⎜⎝

⎛+=μμ

nfn

pfp

KK

LL

μμ

=3

1

Power: < 2 mW/channelNoise: 2 μV rms (10Hz-20kHz)

Technology (Alcatel-Mietec CMOS 0.7μm): KFNMOS = 3e-28 V2F, KFPMOS = 5e-30 V2F

Flicker noise

NO

ISE

POW

ER

MINIMUM: ⇒

Thermal

noiseHSPICE

PRODUCTION

MEASUREMENT

M1: 1500/2 M3: 100/24

.....

BANDPASS FILTER

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

AC coupling – NEURO64

WEAKINVERSION

STRONGINVERSION

R ⇒ GΩ !

Cs = 4pF

Measurements f=10 mHzSimulations

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

CROSSTALK PROBLEM:analogue multiplexer

(input noise VIN-rms < 5 μV rms)

Multiplexer in NEURO64 ⇒ to reduce crosstalk

Referencechannel

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Matching

Measure parameters

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Example of practical application:RETINAL READOUT SYSTEM

Four group of people from:UC - Santa Cruz: data acquisition system & analysisAGH UST - Krakow: IC design and testingUniv. Glasgow – UK: microelectrode fabricationSalk Institute - San Diego: neurobiology

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Experimental set-upRETINAL READOUT SYSTEM

A movie is focused on the retina tissue

⇓The patterns of electrical activity generated by hundreds of retinal

output neurons are recorded

Experiments have been done in:Salk Institute, San Diegohttp://www.snl-e.salk.edu

Retinal tissue placed on top of mulielectrode array

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Working system with 512 readout channels

To understand how the retina processes and encodes dynamic visual image

Out

put v

olta

ge [m

V]

Time [ms]

Fragment modułu512-kanałowy

NEURO64

PLAT64

"pitch adaptor"

512 electrodeswith retina tissue

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Electrodespike-rate

Spike-rate forOn-off DS

neurons

Spike-rate forOn-off DS

neurons

2 mm

Tests with the monkey retina – moving bar(Litke, et. al.)

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Additional functionally required:

RECORDING + STIMULATION+TELEMETRY

K. D. Wise et. Al., IEEE TBE 2004

IDEAL SYSTEM

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

RP - RetinisPigmentosa

( 12 mln people)

Effect of Effect of RetinaRetina DiseasesDiseases..

Normal Macular Degeneration (AMD)

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

System MIT/Harvard(epiretinal implant)

Optiobionics Corporation(subretinal implant)

ASR: 2 mm x 25 um5000 pixels,: 20 um x 20 um

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

NeuroNexus Technologies

Deep brain stimulation – microprobes

Next step - MEMS

S P↓N S W↑T C H Workshop „Spin Momentum Transfer” , Kraków 2008

Summary