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Try to save computation time in largescale neural network modeling with population density methods,

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Title: Try to save computation time in largescale neural network modeling with population density methods,


1
Try to save computation time in large-scale
neural networkmodeling with population density
methods, or just fuhgeddaboudit?
  • Daniel Tranchina, Felix Apfaltrer Cheng Ly
  • New York University
  • Courant Institute of Mathematical Sciences
  • Department of Biology
  • Center for Neural Science
  • Supported by NSF grant BNS0090159

2
  • SUMMARY
  • Can the population density function (PDF) method
    be made into a practical time-saving
    computational tool in large-scale neural network
    modeling?
  • Motivation for thinking about PDF methods
  • General theoretical and practical issues
  • The dimension problem in realistic single-neuron
    models
  • Two dimension reduction methods
  • Moving eigenfunction basis (Knigh, 2000)
  • only good news
  • Moment closure method (Cai et al., 2004)
  • good news bad news worse news good news
  • Example of a model neuron with a 2-D state space
  • Future directions

3
  • Why Consider PDF Methods in Network Modeling?
  • Synaptic noise makes neurons behave
    stochastically synaptic failure random sizes of
    unitary events random synaptic delay.
  • Important physiological role mechanism for
    modulation of gain/kinetics of population
    responses to synaptic input prevents synchrony
    in spiking neuron models as in the brain.
  • Important to capture somehow the properties of
    noise in realistic models.
  • Large number of neurons required for modeling
    physiological phenomena of interest, e.g. working
    memory orientation tuning in primary visual
    cortex.

4
Why Consider PDF Methods (continued)
  • Number of neurons is determined by the functional
    subunit e.g. an orientation hypercolumn in V1
  • TYPICAL MODELS (1000 neurons)/(orientation
    hypercolumn) for input layer V1 ( 0.5 X 0.5 mm2
    or roughly 0.25 X 0.25 deg2 ).
  • REALITY 34,000 neurons, 75 million synapses
  • Many hypercolumns are required to study some
    problems, e.g. dependence of spatial integration
    area on stimulus contrast.

5
  • Why PDF? (continued)
  • Tracking by computation the activity of 103--104
    neurons and 104--106 synapses taxes
    computational resources time and memory.
  • e.g. 8 X 8 hypercolumn-model for V1 with
    64,000 neurons
  • (Jim Wielaard and collaborators, Columbia)
  • 1 day to simulate 4 seconds real time
  • But stunning recent progress by Adi Rangan
    David Cai

What to do? Quest for the Holy Grail a
low-dimensional system of equations that
approximates the behavior of a truly
high-dimensional system. Firing rate model (Dyan
Abbott, 2001) system of ODEs or PDF model
(system of PDEs or integro-PDEs)?
6
  • The PDF Approach
  • Large number of interacting stochastic units
    suggests a statistical mechanical approach.
  • Lump similar neurons into discrete groups.
  • Example V1 hypercolumn. Course graining over
    position, orientation preference receptive-field
    structure (spatial-phase) simple--complex E vs.
    I may give 50 neurons/population ( tens OK for
    PDF methods).
  • Each neuron has a set of dynamical variables that
    determines its state e.g.

for a leaky IF neuron.
  • Track the distribution of neurons over state
    space and firing rate for each population.

7
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8
PDF Theory
9
Minimal IF Model How Many State Variables?
10
Take Baby Steps Introduce Dimensions One at a
Time and See What We Can Do
11
v nullcline
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13
PDF vs. MC and Mean-Field for 2-D Problem. PDF
cpu time is 400 single uncoupled neurons
MC
1000 neurons
PDF
mean-field
100,000 neurons
cpu time 0.8 s for PDF 2 s per 1000 neurons for
MC.
14
Computation Time Comparison PDF vs. Monte Carlo
(MC) PDF grows linearly MC grows quadratically
50 neurons per population1 run 25 connectivity
15
  • PDF Method is plenty fast for model neurons with
    a 2-D state space.
  • More realistic models (e.g. with E and I input)
    require additional state variables
  • Explore dimension reduction methods.
  • Use the 2-D problem as a test problem

16
Dimension Reduction by Moving Eigenvector
Basis Bowdlerization of Bruce Knights (2000)
Idea
17
Dimension Reduction by Moving Eigenvector
Basis Example with 1-D state space, instantaneous
synaptic kinetics
  • Only 3 eigenvectors for low, and 7 for high
    synaptic input rates.
  • Large time steps
  • Eigen-method is 60 times faster than full 1-D
    solution

Suggested by Knight, 2000.
18
Dimension Reduction by Moving Eigenvector
Basis Example with 2-D state space state
variables V Ge
  • Out of 625 eigenvectors 10 for high, 30 for
    medium, and 60 for low synaptic input rates.
  • Large time steps
  • Eigen-method is 60 times faster than full 1-D
    solution

19
Dimension Reduction by Moment Closure
20
Dimension Reduction by Moment Closure 2nd Moment
Stimulus
Firing Rate Response
Near perfect agreement between results from
dimension reduction by moment closure, and full
2-D PDF method.
21
Dimension Reduction by Moment Closure 3rd Moment
Response to Square-Wave Modulation of Synaptic
Input Rate
3rd-moment closure performs better than 2nd at
high input rates.
22
Trouble with Moment Closure and Troubleshooting
  • Dynamical solutions breakdown when synaptic
    input rates drop below 1240 Hz, where actual
    firing rate (determined by MC and full 2-D
    solution) 60 spikes/s.
  • Numerical problem or theoretical problem?
  • Is moment closure problem ill-posed for some
    physiological parameters?
  • Examine the more tractable steady-state problem

23
Steady-State Moment Closure Problem Existence
Study
24
Phase Plane Analysis of Steady-State Moment
Closure Problem to Study Existence/Nonexistence
of Solutions
25
Phase Plane and Solution at High Synaptic Input
Rate
solution trajectory
must intersect
26
Steady-State Solution Doesnt Exist for Low
Synaptic Input Rate
27
Promise of a New Reduced Kinetic Theory with
Wider Applicability, Using Moment Closure
A numerical method on a fixed voltage grid that
introduces a boundary layer with numerical
diffusion finds solutions in good agreement with
direct simulations.
(Cai, Tao, Shelley, McLaughlin, 2004)
28
SUMMARY
  • PDF methods show promise
  • Small population size OK, but connectivity cannot
    be dense
  • Realistic synaptic kinetics introduce state-space
    variables
  • Time saving benefit lost when state space
    dimension is high
  • Dimension reduction methods could maintain
    efficiency
  • Moving eigenvector basis speeds up 2-D PDF
    method 60 X
  • Moment closure method (unmodified) has existence
    problems
  • Numerical implementations suggest moment closure
    can work well
  • Challenge is to find methods that work for gt 3
    dimensions

29
THANKS
  • Bruce Knight
  • Charles Peskin
  • David McLaughlin
  • David Cai
  • Adi Rangan
  • Louis Tao
  • E. Shea-Brown
  • B. Doiron
  • Larry Sirovich

30
Edges of parameter space
Minimal input rate
Minimal EPSP with fixed mean G
fix at mean-field threshold, increase
EPSP ( ) until solution exists
31
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33
Parameter Values
34
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35
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