Title: Dynamical network motifs: building blocks of complex dynamics in biological networks
1Dynamical network motifsbuilding blocks of
complex dynamics in biological networks
- Valentin Zhigulin
- Department of Physics, Caltech, and
- Institute for Nonlinear Science, UCSD
2Spatio-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
3Challenges 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
4Questions
- How can we understand the influence of networks
structure on their dynamics? - Can we predict dynamics in networks from the
topology of their connectivity?
5Simple dynamical model
6Hopfield (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
7Networks 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
8Further simplifications of the model
9Dynamics in a simple circuit
- Single, input-dependent attractor
- Robust, reproducible dynamics
- Fast convergence regardless of initial conditions
10LLE lt 0
LLE 0
LLE gt 0
11Studying 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
12Dynamical 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
13Hypothesis 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 -
14Testing 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
15Motifs with periodic dynamics (LLE0)
3 nodes, 3 links -
4 nodes, 5 links -
16Motifs with chaotic dynamics (LLEgt0)
5 nodes 9 links
7 nodes 10 links
8 nodes 11 links
6 nodes 10 links
17Appearance of dynamical motifs in random networks
18Appearance of dynamical motifs II
19Prediction of the transition in random networks
20Appearance of chaotic motifs
21How 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
222D model of a spatially distributed network
23Dynamics 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
24Number of motifs in spatial networks
25Computations in a model of a cortical microcircuit
Maass, Natschläger, Markram, Neural Comp., 2002
26Take-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.
27Acknowledgements
- 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)