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Dynamical network motifs: building blocks of complex dynamics in biological networks

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Title: Dynamical network motifs: building blocks of complex dynamics in biological networks


1
Dynamical network motifsbuilding blocks of
complex dynamics in biological networks
  • Valentin Zhigulin
  • Department of Physics, Caltech, and
  • Institute for Nonlinear Science, UCSD

2
Spatio-temporal dynamics in biological networks
  • Periodic oscillations in cell-cycle regulatory
    network
  • Periodic rhythms in the brain
  • Chaotic neural activity in models of cortical
    networks
  • Chaotic dynamics of populations sizes in food
    webs
  • Chaos in chemical reactions

3
Challenges for understanding of these dynamics
  • Strong influence of networks structure on their
    dynamic
  • It induces long term, connectivity-dependent
    spatio-temporal correlations which present
    formidable problem for theoretical treatment
  • These correlations are hard to deal with because
    connectivity is in general not symmetric, hence
    dynamics is non-Hamiltonian
  • Dynamical mean field theory may allow one to
    solve such a problem in the limit of
    infinite-size networks Sompolinsky et al,
    Phys.Rev.Lett. 61 (1988) 259-262
  • However, DMF theory is not applicable to the
    study of realistic networks with non-uniform
    connectivity and a relatively small size

4
Questions
  • How can we understand the influence of networks
    structure on their dynamics?
  • Can we predict dynamics in networks from the
    topology of their connectivity?

5
Simple dynamical model
6
Hopfield (attractor) networks
  • Symmetric connectivity ? fixed point attractors
  • Memories (patterns) are stored in synaptic
    weights
  • Current paradigm for the models of working
    memory

There is no spatio-temporal dynamics in the model
7
Networks with random connectivity
  • For most biological networks exact connectivity
    is not known
  • As a null hypothesis, let us first consider
    dynamics in networks with random (non-symmetric)
    connectivity
  • Spatio-temporal dynamics is now possible
  • Depending on connectivity, periodic, chaotic and
    fixed point attractors can be observed in such
    networks

8
Further simplifications of the model
9
Dynamics in a simple circuit
  • Single, input-dependent attractor
  • Robust, reproducible dynamics
  • Fast convergence regardless of initial conditions

10
LLE lt 0
LLE 0
LLE gt 0
11
Studying dynamics in large random networks
  • Consider a network of N nodes with some
    probability p of node-to-node connections
  • For each p generate an ensemble of 104p
    networks with random connections ( pN2 links)
  • Simulate dynamics in each networks for 100 random
    initial conditions to account for possibility of
    multiple attractors in the network
  • In each simulation calculate LLE and thus
    classify each network as having chaotic (at least
    one LLEgt0), periodic (at least one LLE0 and no
    LLEgt0) or fixed point (all LLEslt0) dynamics
  • Calculate F (fraction of an ensemble for each
    type of dynamics) as a function of p

12
Dynamical transition in the ensemble
  • Similar transitions had been observed in models
    of genetic networks Glass and Hill, Europhys.
    Lett. 41 599 and balanced neural networks van
    Vreeswijk and Sompolinsky, Science 274 1724

13
Hypothesis about the nature of the transition
  • As more and more links are added to the network,
    structures with non-trivial dynamics start to
    form
  • At first, subnetworks with periodic dynamics and
    then subnetworks with chaotic dynamics appear
  • The transition may be interpreted as a
    proliferation of dynamical motifs smallest
    dynamical subnetworks

14
Testing the hypothesis
  • Strategy
  • Identify dynamical motifs - minimal subnetworks
    with non-trivial dynamics
  • Estimate their abundance in large random networks
  • Roadblocks
  • Number of all possible directed networks growth
    with their size n as 2n2
  • Rest of the network can influence motifs
    dynamics
  • Simplifications
  • We can estimate the number of active elements in
    the rest of the network and make sure that they
    do not suppress motifs dynamics
  • Number of non-isomorphic directed networks grows
    much slower
  • Since the probability to find a motif with l
    links in a random network is proportional to pl,
    we are only interested in motifs with small
    number of links

15
Motifs with periodic dynamics (LLE0)
3 nodes, 3 links -
4 nodes, 5 links -
16
Motifs with chaotic dynamics (LLEgt0)
5 nodes 9 links
7 nodes 10 links
8 nodes 11 links
6 nodes 10 links
17
Appearance of dynamical motifs in random networks
18
Appearance of dynamical motifs II
19
Prediction of the transition in random networks
20
Appearance of chaotic motifs
21
How to avoid chaos ?
  • Dynamics in many real networks are not chaotic
  • Networks with connectivity that minimizes the
    number of chaotic motifs would avoid chaos
  • For example, brains are not wired randomly, but
    have spatial structure and distance-dependent
    connectivity
  • Spatial structure of the network may help to
    avoid chaotic dynamics

22
2D model of a spatially distributed network
23
Dynamics in the 2D model
  • Only 1 of networks with ?2 exhibit chaotic
    dynamics
  • 99 of networks with ?10 exhibit chaotic
    dynamics
  • Calculations show that chaotic motifs are absent
    in networks with local connectivity (?2) and
    present in non-local networks (?10)
  • Hence local clustering of connections plays an
    important role in defining dynamical properties
    of a network

24
Number of motifs in spatial networks
25
Computations in a model of a cortical microcircuit
Maass, Natschläger, Markram, Neural Comp., 2002
26
Take-home message
Calculations of abundance of dynamical motifs in
networks with different structures allows one to
study and control dynamics in these networks by
choosing connectivity that maximizes the
probability of motifs with desirable dynamics and
minimizes probability of motifs with unacceptable
dynamics. This approach can be viewed as one of
the ways to solve an inverse problem of inferring
network connectivity from its dynamics.
27
Acknowledgements
  • Misha Rabinovich (INLS UCSD)
  • Gilles Laurent (CNS Biology, Caltech)
  • Michael Cross (Physics, Caltech)
  • Ramon Huerta (INLS UCSD)
  • Mitya Chklovskii (Cold Spring Harbor Laboratory)
  • Brendan McKay (Australian National University)
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