SlideShare a Scribd company logo
Latency of Thalamocortical Fast-Spiking
Interneurons in Schizophrenia
Jennifer Houser
East Tennessee State University
July 24, 2014
Jennifer Houser Mathematical Biosciences Institute 2014 REU
Overview
Topics
MATLAB Modeling
Voltage-Gated Ion Channels
Spiking Neurons
Delay Differential Equations
Integrate-and-Fire Model
Future Work
Jennifer Houser Mathematical Biosciences Institute 2014 REU
Voltage-Gated Ion Channels
Models ionic channel gating variables
Recall that the conductance of an ionic channel is equal to the
probability that the channel is open
Rate at which a channel is open is related to the difference
between the probability of a closed channel being opened and the
probability of an open channel being closed
dw
dt = (1 − w)k1 − wk2 = k1 − (k1 + k2)w, for w = n, m, h
Input arguments: membrane potential and current probability that
the ionic channel is open
Simplistic but requires numerical data as input
P. Wallisch, M. E. Lusignan, M. D. Benayoun, T. I. Baker, A. S. Dickey, and N. G. Hatsopoulos, MATLAB for Neuroscientists.
Academic Press, London, 2014.
Jennifer Houser Mathematical Biosciences Institute 2014 REU
Spiking Neuron Model
System of two ordinary-differential equations and a reset condition
developed by E. Izhikevich
dv
dt
= 0.04v2
+ 5v + 140 − u + I
du
dt
= a(bv − u)
If v ≥ 30, then c → v and u + d → u
v: membrane potential
u: membrane recovery variable
Accounts for activation of K+
channels and inactivation of Na+
channels
E. M. Izhikevich. Simple model of spiking neurons. IEEE Transactions on Neural Networks. 14: 1569-1572, 2003.
Jennifer Houser Mathematical Biosciences Institute 2014 REU
Regular Spiking Neuron Plot
P. Wallisch, M. E.
Lusignan, M. D. Benayoun, T. I. Baker, A. S. Dickey, and N. G. Hatsopoulos, MATLAB for Neuroscientists. Academic Press,Jennifer Houser Mathematical Biosciences Institute 2014 REU
Fast Spiking Neuron Plot
P. Wallisch, M. E.
Lusignan, M. D. Benayoun, T. I. Baker, A. S. Dickey, and N. G. Hatsopoulos, MATLAB for Neuroscientists. Academic Press,Jennifer Houser Mathematical Biosciences Institute 2014 REU
Delayed Differential Equations (DDE)
dx
dt
= f(x(t), x(t − τ))
Rate of change of event at some current time is dependent on the
behavior of the function at some previous
Models various time processes or stage events such as:
Maturation of a species from newborn to adolescent
Delayed birth rate
State variable x must correspond to the interval [t − τ, t], τ > 0
The equation requires initial values for x(t0) and x(t0 − τ)
MATLAB built-in solver for DDE
dde23
J. E. Forde. (2005) Delay differential equation models in mathematical biology (Unpublished doctoral dissertation). The University
Jennifer Houser Mathematical Biosciences Institute 2014 REU
Integrate-and-Fire Models
Does not take into account the underlying mechanisms of action
potentials
Utilizes a threshold value for the membrane potential that triggers
an action potential
vth
Membrane potential is reset to subthreshold level after the
occurrence of an action potential
vr
Ability to incorporate refractory period
tref
Jennifer Houser Mathematical Biosciences Institute 2014 REU
Leaky Integrate-and-Fire (LIF) Model
τm
dv
dt
= −v(t) + RI(t)
v(t): membrane potential as a function of time
τm: membrane time constant
R: resistance
I(t): current as a function of time
Simplest form of LIF model
Easy to compute numerically and analytically
Jennifer Houser Mathematical Biosciences Institute 2014 REU
Extensions of LIF Model
Include a refractory period involving a delay in the action potential
once the membrane potential has been reset
Constant input current: I(t) = I
Models periodic behavior of action potentials
Time-varying input current: I(t)
Describes the membrane potential between action potential
occurrences
Synaptic currents
Describes the spiking behavior due to pre-synaptic currents
Considers the summation of individual pre-synaptic events
M. Beierlein, J. R. Gibson, and B. W. Connors. ”Two dynamically distinct inhibitory networks in layer 4 of the neocortex.” J.
Neurophsiol., 90: 2987 - 3000, 2003.
Jennifer Houser Mathematical Biosciences Institute 2014 REU
Future Work
Short-Term Goals
Study integrate-and-fire model
Further investigate the mechanisms of the feed-forward inhibition
circuit
Develop mathematical model to represent feed-forward inhibition
Learn how to incorporate latency into model
Long-Term Goals
Write model section of paper
Incorporate a latency term in model
Jennifer Houser Mathematical Biosciences Institute 2014 REU

More Related Content

PPTX
Question 2 media
PDF
CIRTEMO_Overview_with hyperspectral example-Pre-NDA
PDF
SungardASRaaS_WhitePaper_Final
PPTX
Social Media Marketing for Local Business - Presentation to BNI Williamstown,...
PDF
Jck mag
PDF
RS Procurement Ebook
PPTX
CPD-Y - Senior Seminar (2)
PPTX
Question 3
Question 2 media
CIRTEMO_Overview_with hyperspectral example-Pre-NDA
SungardASRaaS_WhitePaper_Final
Social Media Marketing for Local Business - Presentation to BNI Williamstown,...
Jck mag
RS Procurement Ebook
CPD-Y - Senior Seminar (2)
Question 3

Viewers also liked (6)

PPTX
qubesocial Hobsons Bay Local Social Media Marketing Presentations
PDF
Project pheme pitch deck
PPTX
Arka Kalpana
DOCX
Ta .WANIMBO
PPTX
Intellectual property rights in India with special reference to Patent
PDF
CV-Eng.Sarah
qubesocial Hobsons Bay Local Social Media Marketing Presentations
Project pheme pitch deck
Arka Kalpana
Ta .WANIMBO
Intellectual property rights in India with special reference to Patent
CV-Eng.Sarah
Ad

Similar to NeuronsPart4 (20)

PPTX
The Missing Fundamental Element
PPT
neuronal network of NS systems short.ppt
PPTX
What is different about life? it is inherited oberwolfach march 7 1 2018
PPTX
Penn state cam lecture february 2015
PPTX
Device approach to biology and engineering
PPTX
Talk device approach to biology march 29 1 2015
DOCX
Ion Channel Simulations for Potassium, Sodium, Calcium, and Chloride Channels...
PDF
JMM_Poster_2015
PPTX
Memristive behavior in nanoscale
PPT
Neural Engineering Research Overview
PDF
CAD Simulation of ion channels
PDF
CV of Md Nasir Uddin Bhuyian
PPT
Hodgkin-Huxley & the nonlinear dynamics of neuronal excitability
DOCX
PNP what is in a name july 25 1 2019
PDF
Averitt slides
PPTX
Research Poster
PPTX
Ion-acoustic rogue waves in multi-ion plasmas
PDF
DPG_Talk_March2011_AlexandraM_Liguori
PPTX
Doctorate Thesis Presentation
The Missing Fundamental Element
neuronal network of NS systems short.ppt
What is different about life? it is inherited oberwolfach march 7 1 2018
Penn state cam lecture february 2015
Device approach to biology and engineering
Talk device approach to biology march 29 1 2015
Ion Channel Simulations for Potassium, Sodium, Calcium, and Chloride Channels...
JMM_Poster_2015
Memristive behavior in nanoscale
Neural Engineering Research Overview
CAD Simulation of ion channels
CV of Md Nasir Uddin Bhuyian
Hodgkin-Huxley & the nonlinear dynamics of neuronal excitability
PNP what is in a name july 25 1 2019
Averitt slides
Research Poster
Ion-acoustic rogue waves in multi-ion plasmas
DPG_Talk_March2011_AlexandraM_Liguori
Doctorate Thesis Presentation
Ad

NeuronsPart4

  • 1. Latency of Thalamocortical Fast-Spiking Interneurons in Schizophrenia Jennifer Houser East Tennessee State University July 24, 2014 Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 2. Overview Topics MATLAB Modeling Voltage-Gated Ion Channels Spiking Neurons Delay Differential Equations Integrate-and-Fire Model Future Work Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 3. Voltage-Gated Ion Channels Models ionic channel gating variables Recall that the conductance of an ionic channel is equal to the probability that the channel is open Rate at which a channel is open is related to the difference between the probability of a closed channel being opened and the probability of an open channel being closed dw dt = (1 − w)k1 − wk2 = k1 − (k1 + k2)w, for w = n, m, h Input arguments: membrane potential and current probability that the ionic channel is open Simplistic but requires numerical data as input P. Wallisch, M. E. Lusignan, M. D. Benayoun, T. I. Baker, A. S. Dickey, and N. G. Hatsopoulos, MATLAB for Neuroscientists. Academic Press, London, 2014. Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 4. Spiking Neuron Model System of two ordinary-differential equations and a reset condition developed by E. Izhikevich dv dt = 0.04v2 + 5v + 140 − u + I du dt = a(bv − u) If v ≥ 30, then c → v and u + d → u v: membrane potential u: membrane recovery variable Accounts for activation of K+ channels and inactivation of Na+ channels E. M. Izhikevich. Simple model of spiking neurons. IEEE Transactions on Neural Networks. 14: 1569-1572, 2003. Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 5. Regular Spiking Neuron Plot P. Wallisch, M. E. Lusignan, M. D. Benayoun, T. I. Baker, A. S. Dickey, and N. G. Hatsopoulos, MATLAB for Neuroscientists. Academic Press,Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 6. Fast Spiking Neuron Plot P. Wallisch, M. E. Lusignan, M. D. Benayoun, T. I. Baker, A. S. Dickey, and N. G. Hatsopoulos, MATLAB for Neuroscientists. Academic Press,Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 7. Delayed Differential Equations (DDE) dx dt = f(x(t), x(t − τ)) Rate of change of event at some current time is dependent on the behavior of the function at some previous Models various time processes or stage events such as: Maturation of a species from newborn to adolescent Delayed birth rate State variable x must correspond to the interval [t − τ, t], τ > 0 The equation requires initial values for x(t0) and x(t0 − τ) MATLAB built-in solver for DDE dde23 J. E. Forde. (2005) Delay differential equation models in mathematical biology (Unpublished doctoral dissertation). The University Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 8. Integrate-and-Fire Models Does not take into account the underlying mechanisms of action potentials Utilizes a threshold value for the membrane potential that triggers an action potential vth Membrane potential is reset to subthreshold level after the occurrence of an action potential vr Ability to incorporate refractory period tref Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 9. Leaky Integrate-and-Fire (LIF) Model τm dv dt = −v(t) + RI(t) v(t): membrane potential as a function of time τm: membrane time constant R: resistance I(t): current as a function of time Simplest form of LIF model Easy to compute numerically and analytically Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 10. Extensions of LIF Model Include a refractory period involving a delay in the action potential once the membrane potential has been reset Constant input current: I(t) = I Models periodic behavior of action potentials Time-varying input current: I(t) Describes the membrane potential between action potential occurrences Synaptic currents Describes the spiking behavior due to pre-synaptic currents Considers the summation of individual pre-synaptic events M. Beierlein, J. R. Gibson, and B. W. Connors. ”Two dynamically distinct inhibitory networks in layer 4 of the neocortex.” J. Neurophsiol., 90: 2987 - 3000, 2003. Jennifer Houser Mathematical Biosciences Institute 2014 REU
  • 11. Future Work Short-Term Goals Study integrate-and-fire model Further investigate the mechanisms of the feed-forward inhibition circuit Develop mathematical model to represent feed-forward inhibition Learn how to incorporate latency into model Long-Term Goals Write model section of paper Incorporate a latency term in model Jennifer Houser Mathematical Biosciences Institute 2014 REU