Nonlinear Dynamics of Cellular and Network Excitability ...rinzel/CMNSS10/Neuronal dyns...

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Nonlinear Dynamics of Cellular and Network Excitability and Oscillations CMNSS10 See review chapters: JR w/ B Ermentrout, 1998 Borisyuk w/ JR, 2005 Slow network oscillations Case study #1: episodic rhythms in developing spinal cord Case study #2: alterations from perceptual ambiguity Exercises #1, #2

Transcript of Nonlinear Dynamics of Cellular and Network Excitability ...rinzel/CMNSS10/Neuronal dyns...

  • Nonlinear Dynamics of Cellular and NetworkExcitability and Oscillations

    CMNSS10

    See review chapters: JR w/ B Ermentrout, 1998Borisyuk

    w/ JR, 2005

    Slow network oscillations

    Case study #1: episodic rhythms in developing spinal cordCase study #2: alterations from perceptual ambiguity

    Exercises #1, #2

  • τe

    dre

    /dt = -re

    + Se

    (aee

    re

    - aei

    ri

    + Ie

    )

    τi

    dri

    /dt

    = -ri

    + Si

    (aie

    re

    – aii

    ri

    + Ii

    )

    Firing rate model (Amari-Wilson-Cowan) for dynamics of excitatory-inhibitory populations.

    ri

    (t), re

    (t) --

    average firing rate (across population and “over spikes”)

    τe

    , τi --

    “recruitment”

    time scale

    Se

    (input) , Si

    (input) –

    input/output relations

    aee

    etc –

    “synaptic weights”

    0

    0.2

    0.4

    0.6

    0.8

    1

    0 0.2 0.4 0.6 0.8 1

  • Modeling the rhythmic dynamics of developing spinal cordJ Rinzel, NYU

    Background -

    network depressionAn ad hoc firing rate modelPredictions/confirmations A specific mechanism for depressionA minimal cell-based network modelMean field model? J Tabak, M O’Donovan, C Marchetti, B Vladimirski

  • Interneurons Retrogradely Labeled By Calcium Dyes Injected Into The Ventrolateral Funiculus (VLF) Are

    Rhythmically Active (A.Ritter, P.Wenner, S.Ho)

    Inject CalciumDye

    LS1

    Optical signals duringrhythmic activity

    VLF

    ventral

    dorsal

    rostral

    caudal

  • Synaptic Potentials Are Transiently Depressed After An Episode Of Spontaneous Activity

    200 ms

    Time (minutes)

    Nor

    mal

    ized

    Am

    plitu

    de

    epis

    ode

    epis

    ode

  • τa a’ = a∞

    (n.a)-a

    Basic Model: mutual excitatory network.Activity level, a(t) ; availability of synaptic input, n

    τa a’ = a∞

    (input)-a

    GABA is depolarizing

  • Spontaneous Rhythmic Episodes Can Be Modeled By An Excitatory Network With ‘Fast’ And ‘Slow’ Depression

    J Neuroscience, 2000.

    τa a’ = a∞

    (s.d.a)-aτd d’ = d∞

    (a)-d

    Network behavior is modeled by three variables

    Network ActivityActivity-dependent Fast depression

    time

    0.8

    0.6

    0.4

    0.2

    30 40 50

    Delayed Fast Depression Leads to Oscillations

    10 20Fast Depression (d)

    1.0

    τs s’ = s∞

    (a)-sActivity-dependent Slow depression

    time100 200 400 500 600

    Fast and Slow Depression ProducesEpisodic Oscillations

    300

    Activity (a)

    Slow Depression (s)

    0.8

    0.6

    0.4

    0.2

    1.0

  • Cycling dynamics: a-d phase plane, s-fixed.

    a

    d

    a

    s

    Prescribed slow back-and-forth s(t) “looks like”

    episodes, but it’s not autonomous.

  • Framework for bursting: fast/slow analysis

    HH model: repetitive firing

    Example: Morris-Lecar

    + IK-Ca…slow dynamics for Ca2+(t)

    Treat Ca as param, z= 1/(1+Ca)With Ca as dynamic, slow “Elliptic”

    bursting

  • Cycling dynamics: a-d phase plane, s-fixed.

    a

    d

    a

    s

    Prescribed slow back-and-forth s(t) “looks like”

    episodes, but it’s not autonomous.

  • a

    s

    OSC: “cycles”

    SS: silent phase

    a-d phase plane, s fixed.Bistable: upper OSC, lower SS

    FAST/SLOW Analysis

    syn’s

    depressing

    syn’s

    recovering

    Full system: s, slow depression

  • “Kick”

    out of Silent Phase => shorter Active Phase.

    Fast/Slow Dissection --

    a-s “phase plane”

  • THEORY EXPERIMENTJ Neuroscience, 2001.

  • mV

    Cl

    influx

    Cl

    efflux

    V_Cl

    V

    FAST/SLOW Analysis

  • N-cell I&F network. w/ J Tabak, B Vladimirski

    All-to-all excitatory coupling. Non-identical cells: I min

    < I j

    < I max

    If I max

    >1 some cells fire spontaneously.

    Slow depression, no cycles.

    J Computl

    Neuro, 2008

  • sj

    vs

    j

    gsyn

    eff

    raster plot

    N-cell I&F network; N=50; Imin=0.1; Imax=1.1I=0 I=1

    OSCEXC

  • Demonstration of bistability:

    Use self-consistency at each t,with current values of {sj

    } –find 3 states: L, M, U…

    U-M coalesce at end of Silent PhaseL-M at end of Active Phase

  • SUMMARY: Modeling of Spontaneous Rhythms Ad hoc Mean Field model:

    Episodic rhythms -

    generated from mutual excitation with slow synaptic depression;

    -

    fast depression yields cycling during episodes.

    Bistability

    of fast subsystem leads to predictions forcorrelations between SP duration and next AP duration.

    GABAA

    synapses are “functionally”

    excitatory, ie

    V < VCl

    ;VCl

    is depolarized and it oscillates together with episodes; minimal model shows it.

    N-cell network model:

    Cycling during AP? Stochastic synapses for initiating next AP?

    Dynamics of heterogeneous network.

    Slide Number 1Slide Number 2Slide Number 3Interneurons Retrogradely Labeled By Calcium Dyes Injected Into The Ventrolateral Funiculus (VLF) Are Rhythmically Active (A.Ritter, P.Wenner, S.Ho)Slide Number 5Slide Number 6Spontaneous Rhythmic Episodes Can Be Modeled By An Excitatory Network With ‘Fast’ And ‘Slow’ Depression� J Neuroscience, 2000.Slide Number 8Slide Number 9Slide Number 10Slide Number 11Slide Number 12Slide Number 13Slide Number 14Slide Number 15Slide Number 16Slide Number 17Slide Number 18Slide Number 19