Theoretical Neuroscience Physics 405, Copenhagen University Block 4, Spring 2007 John Hertz...

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Theoretical NeurosciencePhysics 405, Copenhagen University

Block 4, Spring 2007

John Hertz (Nordita)Office: rm Kc10, NBI Blegdamsvej

Tel 3532 5236 (office) 2720 4184 (mobil)hertz@nordita.dk

www.nordita.dk/~hertz/course.html

Texts: P Dayan and L F Abbott, Theoretical Neuroscience (MIT Press)W Gerstner and W Kistler, Spiking Neuron Models (Cambridge U Press) http://diwww.epfl.ch/~gerstner/SPNM/SPNM.html

Outline

• Introduction: biological background, spike trains• Biophysics of neurons: ion channels, spike generation • Synapses: kinetics, medium- and long-term synaptic

modification• Mathematical analysis using simplified models• Network models:

– noisy cortical networks– primary visual cortex– associative memory– oscillations in olfactory circuits

Lecture I: Introduction

ca 1011 neurons/human brain

104/mm3

soma 10-50 m

axon length ~ 4 cm

total axon length/mm3 ~ 400 m

Cell membrane, ion channels, action potentials

Membrane potential: rest at ca -70 mvNa-K pump maintains excess K inside,Na outside

Na in: V rises,more channels open “spike”

Communication: synapses

Integrating synaptic input:

Brain anatomy: functional regions

Visual system

General anatomy Retina

Neural coding: firing rates depend on stimulus

Visual cortical neuron:variation with orientationof stimulus

Neural coding: firing rates depend on stimulus

Visual cortical neuron:variation with orientationof stimulus

Motor cortical neuron:variation with directionof movement

Neuronal firing is noisy

Motion-sensitive neuron in visual area MT: spike trains evoked by multiplepresentations of moving random-dotpatterns

Neuronal firing is noisy

Motion-sensitive neuron in visual area MT: spike trains evoked by multiplepresentations of moving random-dotpatterns

Intracellular recordings of membrane potential: Isolated neurons fire regularly; neurons in vivo do not:

Quantifying the response of sensory neurons

spike-triggered average stimulus (“reverse correlation”)

Examples of reverse correlation

Electric sensory neuron inelectric fish:s(t) = electric field

Motion-sensitive neuron in blowflyVisual system:s(t) = velocity of moving pattern invisual field

Note: non-additive effect for spikesvery close in time (t < 5 ms

Spike trains: Poisson process model

Homogeneous Poisson process: = rate = prob of firing per unit time,

i.e., prob of spike in interval

rtr )0(),[ tttt

Spike trains: Poisson process model

Homogeneous Poisson process: = rate = prob of firing per unit time,

i.e., prob of spike in interval

rtr )0(),[ tttt

Survivor function: probability of not firing in [0,t): S(t)

Spike trains: Poisson process model

Homogeneous Poisson process: = rate = prob of firing per unit time,

i.e., prob of spike in interval

rtr )0(),[ tttt

Survivor function: probability of not firing in [0,t): S(t)

rttStS

dttdSr

e)(

)(

/)(

Spike trains: Poisson process model

Homogeneous Poisson process: = rate = prob of firing per unit time,

i.e., prob of spike in interval

rtr )0(),[ tttt

Survivor function: probability of not firing in [0,t): S(t)

Probability of firing for the first time in [t, t +t)/ t :

rttStS

dttdSr

e)(

)(

/)(

Spike trains: Poisson process model

Homogeneous Poisson process: = rate = prob of firing per unit time,

i.e., prob of spike in interval

rtr )0(),[ tttt

Survivor function: probability of not firing in [0,t): S(t)

Probability of firing for the first time in [t, t +t)/ t :

rttStS

dttdSr

e)(

)(

/)(

rtrdt

tdStP e

)()(

Spike trains: Poisson process model

Homogeneous Poisson process: = rate = prob of firing per unit time,

i.e., prob of spike in interval

rtr )0(),[ tttt

Survivor function: probability of not firing in [0,t): S(t)

Probability of firing for the first time in [t, t +t)/ t :

(interspike interval distribution)

rttStS

dttdSr

e)(

)(

/)(

rtrdt

tdStP e

)()(

Homogeneous Poisson process (2)

Probability of exactly 1 spike in [0,T):

rTtTrT rtT rTrdtP eee)1( )(

0

Homogeneous Poisson process (2)

Probability of exactly 1 spike in [0,T):

rTtTrT rtT rTrdtP eee)1( )(

0

Probability of exactly 2 spikes in [0,T):

rTtTrttrT rtt

T rTrrdtdtP e)(eee)2( 221)()(

0 0 122121

2

Homogeneous Poisson process (2)

Probability of exactly 1 spike in [0,T):

rTtTrT rtT rTrdtP eee)1( )(

0

Probability of exactly 2 spikes in [0,T):

rTtTrttrT rtt

T rTrrdtdtP e)(eee)2( 221)()(

0 0 122121

2

… Probability of exactly n spikes in [0,T):

rTnT rT

nnP e)(

!

1)(

Homogeneous Poisson process (2)

Probability of exactly 1 spike in [0,T):

rTtTrT rtT rTrdtP eee)1( )(

0

Probability of exactly 2 spikes in [0,T):

rTtTrttrT rtt

T rTrrdtdtP e)(eee)2( 221)()(

0 0 122121

2

… Probability of exactly n spikes in [0,T):

rTnT rT

nnP e)(

!

1)( Poisson distribution

Poisson distribution

rTn

T nrT

nP e!)(

)(

Pprobability of n spikes in interval of duration T:

Poisson distribution

rTn

T nrT

nP e!)(

)(

Pprobability of n spikes in interval of duration T:

rTn Mean count:

Poisson distribution

rTn

T nrT

nP e!)(

)(

Pprobability of n spikes in interval of duration T:

rTn Mean count:

variance: nrTnn 2)(

Poisson distribution

rTn

T nrT

nP e!)(

)(

Pprobability of n spikes in interval of duration T:

rTn Mean count:

variance: nrTnn 2)( i.e., spikesnn

Poisson distribution

rTn

T nrT

nP e!)(

)(

Pprobability of n spikes in interval of duration T:

rTn Mean count:

variance: nrTnn 2)( i.e., spikesnn

large : GaussianrT

Poisson distribution

rTn

T nrT

nP e!)(

)(

Pprobability of n spikes in interval of duration T:

rTn Mean count:

variance: nrTnn 2)( i.e., spikesnn

large : GaussianrT

Poisson process (2): interspike interval distribution

rtrtP e)(Exponential distribution: (like radioactive Decay)

Poisson process (2): interspike interval distribution

rtrtP e)(

rt

1

Exponential distribution: (like radioactive Decay)

Mean ISI:

Poisson process (2): interspike interval distribution

rtrtP e)(

rt

1

22

2 1)( t

rtt

Exponential distribution: (like radioactive Decay)

Mean ISI:

variance:

Poisson process (2): interspike interval distribution

rtrtP e)(

rt

1

22

2 1)( t

rtt

1mean

devstd CV

Exponential distribution: (like radioactive Decay)

Mean ISI:

variance:

Coefficient of variation:

Poisson process (3): correlation function

)()( f

ftttS Spike train:

Poisson process (3): correlation function

)()( f

ftttS

rtS )(

Spike train:

mean:

Poisson process (3): correlation function

)())()()(()( rrtSrtSC

)()( f

ftttS

rtS )(

Spike train:

mean:

Correlation function:

Stationary renewal processDefined by ISI distribution P(t)

Stationary renewal processDefined by ISI distribution P(t)

Relation between P(t) and C(t):

Stationary renewal process

)())((1

)( 2 trtCr

tC

Defined by ISI distribution P(t)

Relation between P(t) and C(t): define

Stationary renewal process

)())((1

)( 2 trtCr

tC

)'()'(')(

)'()'(')()(

0

0

ttCtPdttP

ttPtPdttPtC

t

t

Defined by ISI distribution P(t)

Relation between P(t) and C(t): define

Stationary renewal process

)())((1

)( 2 trtCr

tC

)'()'(')(

)'()'(')()(

0

0

ttCtPdttP

ttPtPdttPtC

t

t

)()()()( CPPC

Defined by ISI distribution P(t)

Relation between P(t) and C(t): define

Laplace transform:

Stationary renewal process

)())((1

)( 2 trtCr

tC

)'()'(')(

)'()'(')()(

0

0

ttCtPdttP

ttPtPdttPtC

t

t

)()()()( CPPC

)(1)(

)(

P

PC

Defined by ISI distribution P(t)

Relation between P(t) and C(t): define

Laplace transform:

Solve:

Fano factor

1

)( 2

Fnnn

F spike count variance / mean spike count

for stationary Poisson process

Fano factor

1

)( 2

Fnnn

F

dCTtStSdtdtn

rTdttSn

T T

T

)()'()(')(

)(

0 0

2

0

spike count variance / mean spike count

for stationary Poisson process

Fano factor

1

)( 2

Fnnn

F

dCTtStSdtdtn

rTdttSn

T T

T

)()'()(')(

)(

0 0

2

0

r

dC

F

)(

spike count variance / mean spike count

for stationary Poisson process

Fano factor

1

)( 2

Fnnn

F

dCTtStSdtdtn

rTdttSn

T T

T

)()'()(')(

)(

0 0

2

0

r

dC

F

)(

2CVF

spike count variance / mean spike count

for stationary Poisson process

for stationary renewal process (prove this)

Nonstationary point processes

Nonstationary point processes

Nonstationary Poisson process: time-dependent rate r(t)

Still have Poisson count distribution, F=1

Nonstationary point processes

Nonstationary Poisson process: time-dependent rate r(t)

Still have Poisson count distribution, F=1

Nonstationary renewal process: time-dependent ISI distribution

)()(0

tPtP t = ISI probability starting at t0

Experimental results (1)

Correlation functions

Experimental results (1)

Correlation functions Count variance vs mean

Experimental results (2)

ISI distribution

Experimental results (2)

ISI distribution CV’s for many neurons

homework

• Prove that the ISI distribution is exponential for a stationary Poisson process.

• Prove that the CV is 1 for a stationary Poisson process.• Show that the Poisson distribution approaches a Gaussian one for

large mean spike count.

• Prove that F = CV2 for a stationary renewal process.

• Show why the spike count distribution for an inhomogeneous Poisson process is the same as that for a homogeneous Poisson process with the same mean spike count.