Title: Multiple rhythmic states in a model respiratory CPG
1Multiple 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
2Goal 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
3three examples of central pattern generators
(CPGs)
1) half-center oscillator (Brown, 1911)
components not intrinsically rhythmic generates
repetitive activity without time-dependent drive
42) locomotor CPG (model) Rybak et al., J.
Physiol., 2006
see also Golubitsky, Stewart, et al.
53) 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
7time courses for half-center oscillations from 3
mechanisms persistent sodium, post-inhibitory
rebound (T-current), adaptation (Ca/K-Ca)
8asymmetric drive simulation results
intermediate
adaptation
9asymmetric drive results (cont.)
highly tunable
robust
high phase independence
Daun, Rubin, and Rybak, JCNS, 2009
10Iinh 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
11analysis I. escape vs. release
inhibition off
inhibition off
inhibition on
inhibition on
Skinner et al., Biol. Cybernetics, 1994
121) persistent sodium current escape
Daun, Rubin, and Rybak, JCNS, 2009
132) postinhibitory rebound release
143) adaptation escape release
synaptic threshold
15analysis 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
162) post-inhibitory rebound release
inhibition on
similar durations despite very different drives
baseline drive
baseline orbit
inhibition off
extra drive
173) adaptation escape release
zero inhibition critical point
max inhibition critical point
increasing drive
183) 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
20large network simulations capture multiple rhythms
21activity-based computational model 4 cells, 4
slow variables, voltage-dependent coupling
FAST
excitatory kernel
i 2,3,4 inhibitory cells
SLOW
22three-phase rhythm
23only features two fast jumps
24projection to two-parameter (i.e., slow variable)
plane shows role of escape
release
25can explain frequency effects of changes in
drives to different cells by effects on
escape/release
26multiple rhythms (see MS88, Wed., 10 AM)
27summary
- 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