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Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

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Page 1: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Physiology-based modeling and quantification of auditory evoked

potentials

Cliff Kerr Complex Systems Group

School of Physics, University of Sydney

Page 2: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Introduction

• Aim: to develop a physiology-based method of evoked potential (EP) analysis, in order to:– Provide a means to quantify EPs– Relate EP data to brain physiology

• Implementation: biophysical modeling and deconvolution of EEG data

Page 3: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Outline• What are evoked potentials?• Fitting:

– Methods: theory, data, implementation

– Results: group average waveforms – Application: arousal

• Deconvolution:– Motivation– Theory– Results: synthetic and experimental

data

• Discussion and summary• Challenges and future directions

Page 4: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

What are EPs?

V(V)

t(s)

EEG:

EP:

V(V)

t(s)

Time-locked averaging

stimulus:

Page 5: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Traditional analysis: scoring

Feature Amplitude

Latency Feature Amplitude

Latency

P50 1.2 mV 56 ms

N1 8.0 mV 120 ms

P2 -8.0 mV 264 ms

N1 6.5 mV 112 ms

N2 3.4 mV 224 ms

P3 -19.6 mV 320 ms

Standard Target

Page 6: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

e

i

r

s

n

Cortex

Thalamus

Brainstem

Theory

Page 7: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

• Physiology-based continuum modeling: uses 11 vs. 1,000,000,000,000,000 connections

• Five populations of neurons: – Sensory (excitatory; labeled n)

– Cortical (excitatory & inhibitory; e & i )

– Thalamic relay (excitatory; s)

– Thalamic reticular (inhibitory; r)

• Five neuronal loops: – cortical (Gee , Gei )

– thalamic (Gsrs )

– thalamocortical (Gese , Gesre)

e

i

r

s

n

Theory

Page 8: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Theory

• Model has 14 parameters: – 5 for neuronal coupling strength (Gee , Gei , Gese , Gesre ,

Gsrs )

– 4 for neuronal network properties (, , , t0)

– 5 for stimulus properties (tos , ts , ros , rs)

• Most important parameters are the gains Gab

(coupling strength between neuron populations)

• Model describes conversion process (auditory stimulus → neuronal activity → scalp electrical field) using an analytic transfer function e/n:

n

einout SS

Page 9: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Theory

• Direct impulse:

• Cortical modulation:

• Corticothalamic modulation:

• Transfer function:

srs

esnti

GL

GLeI

2

22/

1

0

eeeiec LGLGDM )1(

srs

esreeseti

t GL

GLGLeM

2

32

1

)(0

tcn

e

MM

IT

),(

),(),(

k

kk

Page 10: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Theory

• Impulse:

• Time-domain impulse response:

kkkr k 23

dd),(),()2(

1),(

tiri

n eeTtR

2

||

2

122

2),(

s

r

s

t

tt

n r

e

t

et

s

os

s

os

rr

r

Page 11: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Data• Sampled from 1527 normal

subjects:– Aged 6-80 years

– Equal numbers male & female

– No neurological diseases, chemical dependencies, etc.

• Stimulus: 1 tone/second for 6 minutes (280 standard tones, 80 target tones)

• Used to produce group average standard and target EPs (generated using >100,000 single trials!)

Page 12: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

2

P1

P2

.

Fitting1) Initial parameters are chosen

Page 13: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

2

P1

P2

.

Fitting2) Gradient descent algorithm reduces 2

of fit

Page 14: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

2

P1

P2

Fitting3) Process is repeated using different

initialisations

Page 15: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

• Excellent fits to standards (up to 400 ms)

Results

Page 16: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

• Excellent fits to targets (up to 300 ms)

Results

Page 17: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Results• Possible changes in neuronal network

properties:

Page 18: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Results• Probable changes in neuronal coupling

strengths:

Page 19: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Results• Definite changes in stability parameters:

Page 20: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Application: arousal

task du

ratio

n (m

in)

0.1 s

-5 μV

0

6

4

2

• Same task (auditory oddball)

• 43 subjects

• Averaged over ten time intervals of 40 seconds each

Page 21: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Application: arousal• Increased cortical activity → decreased

acetylcholine?

Page 22: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Deconvolution: motivation• In model,

thalamocortical loop → N2 feature of targets

• Could target response = standard response + delayed standard response?

Page 23: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Deconvolution: motivation

Page 24: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Theory• Assumption: responses are product of

task-dynamic and task-invariant properties:

• Fourier transform:

• Take the ratio of the two:

• Inverse Fourier transform to get the result:

)]()([)( 1 IDtR SSF )]()([)( 1 IDtR TT

F

)()()]([ IDtR SS F )()()]([ IDtR TT F

)()(

)(

)()(

)()(

CS

T

S

T DD

D

ID

ID

)()]([1 tDD CC F

Page 25: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Theory• Direct deconvolution is uselessly noisy:

• Hence, use Wiener deconvolution:

NSRR

R

R

RD

S

S

S

TC 2

2

|)(|

|)(|

)(

)()(

Page 26: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Synthetic data

Page 27: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Group average data

Page 28: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Single-subject data

Page 29: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Discussion and summary

• Physiology-based EP fitting can be achieved

• Offers significant advantages over traditional methods

• Results tentatively suggest physiology underlying stimulus perception:– Increase in stability: required for a transient

response

– Arousal determined by thalamocortical activity: standards show increased inhibition, targets show increased excitation

– Standards generated by ≈1 thalamocortical impulse, targets by ≈2

Page 30: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Challenges• Fitting challenges

– Degeneracy– Constraints– Testability

• Deconvolution challenges– Noise and artifact– What are we looking for?

• Physiological challenges– Only 1D information– What’s signal?

Page 31: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Future directions• How does the brain change with age?

Standard Target

Page 32: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Future directions• Can our model account for depression?

Page 33: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Future directions• Modeling the ERP “zoo”

– modality

– arousal

– disease

– drugs

Visual: Somatosensory:

Bipolar: Radiculopathy:

Carbonyl sulfide:

Ecstasy:

Quiet sleep:Oddball:

Page 34: Physiology-based modeling and quantification of auditory evoked potentials Cliff Kerr Complex Systems Group School of Physics, University of Sydney

Acknowledgements

Chris J. Rennie

Peter A. Robinson

Jonathon M. Clearwater

Andrew H. Kemp

Brain Resource Ltd.