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Multiple rhythmic states in a model respiratory CPG

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Title: Multiple rhythmic states in a model respiratory CPG


1
Multiple rhythmic states in a model respiratory
CPG
SIAM Conference on Applications of Dynamical
Systems May 19, 2009
Contributors Ilya Rybak, Natalia Shevtsova
Drexel Univ. College of Medicine Jeffrey Smith
NIH Silvia Daun, Bard Ermentrout, Jonathan
Rubin Univ. of Pittsburgh
Silvia Gruhn Univ. Köln
funding NIH, U.S. National Science Foundation
2
Goal to understand the mechanisms of rhythm
generation, and modulation, in the mammalian
respiratory pacemaker network and other central
pattern generators (CPGs)
  • Outline
  • Brief introduction to CPGs
  • Transition mechanisms in inhibitory networks
  • -- review
  • -- changes in drives to CPG components
  • Respiratory network dynamics

3
three examples of central pattern generators
(CPGs)
1) half-center oscillator (Brown, 1911)
components not intrinsically rhythmic generates
repetitive activity without time-dependent drive
4
2) locomotor CPG (model) Rybak et al., J.
Physiol., 2006
see also Golubitsky, Stewart, et al.
5
3) cortex (Yuste et al., Nat. Rev. Neurosci.,
2005)
6
  • idea
  • CPGs feature alternation of 2 synch. cell
    groups
  • similar rhythms may arise from different
    mechanisms
  • mechanisms determine responses to changes in
    drive to 1 or more groups
  • strategy compare 3 half-center relaxation
    oscillator CPG models, featuring 3 different
    rhythmic mechanisms
  • analyze change in period with change in drive to
    both cells and independent phase modulation with
    change in drive to one cell (asymmetric drive)

Daun, Rubin, and Rybak, JCNS, 2009 also see
Curtu et al., SIADS, 2008
7
time courses for half-center oscillations from 3
mechanisms persistent sodium, post-inhibitory
rebound (T-current), adaptation (Ca/K-Ca)
8
asymmetric drive simulation results
intermediate
adaptation
9
asymmetric drive results (cont.)
highly tunable
robust
high phase independence
Daun, Rubin, and Rybak, JCNS, 2009
10
Iinh s(vpre)(v-vinh)
for vinh lt v lt vexc
Iexc s(vpre)(v-vexc)
where

idea n oscillators n trajectories in
shared 2-d phase plane, not 3n-dimensional phase
space
11
analysis I. escape vs. release
inhibition off
inhibition off
inhibition on
inhibition on
Skinner et al., Biol. Cybernetics, 1994
12
1) persistent sodium current escape
Daun, Rubin, and Rybak, JCNS, 2009
13
2) postinhibitory rebound release
14
3) adaptation escape release
synaptic threshold
15
analysis II. asymmetric drive
baseline orbit
inhibition on
baseline
extra drive
extra drive
  • persistent sodium
  • current escape

baseline drive
inhibition off
short silent phase for cell w/extra drive
16
2) post-inhibitory rebound release
inhibition on
similar durations despite very different drives
baseline drive
baseline orbit
inhibition off
extra drive
17
3) adaptation escape release
zero inhibition critical point
max inhibition critical point
increasing drive
18
3) adaptation escape release (cont.)
synaptic threshold
shortened slightly due to stronger drive, which
promotes escape
prolonged due to delayed adaptation
19
back to respiratory networks (Smith talk, MS57,
10 AM Rubin talk, MS88, Wed., 10 AM)
excitatory preBötC kernel is embedded within
3-component inhibitory ring network
Smith et al., J. Neurophysiol., 2007
Rybak et al., Prog. Brain Res., 2007
Rubin et al., J. Neurophysiol., 2009
20
large network simulations capture multiple rhythms
21
activity-based computational model 4 cells, 4
slow variables, voltage-dependent coupling
FAST
excitatory kernel
i 2,3,4 inhibitory cells
SLOW
22
three-phase rhythm
23
only features two fast jumps
24
projection to two-parameter (i.e., slow variable)
plane shows role of escape
release
25
can explain frequency effects of changes in
drives to different cells by effects on
escape/release
26
multiple rhythms (see MS88, Wed., 10 AM)
27
summary
  • CPGs can exhibit complex rhythmic activity
    patterns
  • Different network components can yield similar
    rhythms
  • Transition mechanisms shape responses to drives
  • Transitions by escape, as with persistent sodium
    current, are optimal for independent phase
    modulation
  • Fast-slow decomposition and parametrization of
    slow dynamics yield transition mechanisms and
    effects of drives in multi-cell, multi-phase
    rhythms
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