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Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance Reading the Secrets of Biological Fluctuations Carl Boettiger UC Davis June 27, 2008 Carl Boettiger, UC Davis Biological Fluctuations 1/21

Reading the Secrets of Biological Fluctuations

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I explore tools and applications of the van Kampen expansion of the stochastic master equation in several areas of population biology. I highlight fluctuation-dissipation and fluctuation-enhancement regimes, using information from noise to help model choice, and examples where noise changes the macroscopic dynamics of a system.

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Page 1: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Reading the Secrets of Biological Fluctuations

Carl Boettiger

UC Davis

June 27, 2008

Carl Boettiger, UC Davis Biological Fluctuations 1/21

Page 2: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

1 Noisy Biology

2 Fluctuation Regimes

3 Model Choice

4 Macroscopic Phenomena

5 Fluctuation Dominance

Carl Boettiger, UC Davis Biological Fluctuations 2/21

Page 3: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Why study fluctuations?

Biology is noisy and we want to understand it.

Stochasticity can drive phenomena we would miss indeterministic models.

Fluctuations hold the key to deeper biological understanding?

Grenfell et al. (1998) Nature

Carl Boettiger, UC Davis Biological Fluctuations 3/21

Page 4: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Variables at the Macroscopic and Individual Levels

Deterministic models describe macroscopic behavior

Individual based model are described by transition ratesbetween states – a Markov process

Macroscopic variable φ is independent of details of system(intensive), i.e. population density

Individual-based variable n depends on system size(extensive), i.e. population number

In a given area Ω with a macroscopic density φ, we’d expectto find 〈n〉 = φΩ on average, which is more accurate withlarger Ω.

Carl Boettiger, UC Davis Biological Fluctuations 4/21

Page 5: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Theory of Fluctuations

Markov process Linear Noise Approximation

=⇒ n = Ωφ+Ω1/2ξ =⇒

Fundamental Equations

dφdt

= α1,0(φ)+α′′1,0(φ)σ2 (1)

dσ2

dt= 2α′

1,0(φ)σ2 + α2,0(φ) (2)

α1,0(φ) = b(φ)− d(φ), α2,0 = b(φ) + d(φ)

Carl Boettiger, UC Davis Biological Fluctuations 5/21

Page 6: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

1 Noisy Biology

2 Fluctuation Regimes

3 Model Choice

4 Macroscopic Phenomena

5 Fluctuation Dominance

Carl Boettiger, UC Davis Biological Fluctuations 6/21

Page 7: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Distinct Fluctuation Regimes

dn

dt= c

n

N

“1− n

N

”| z

bn

− en

N|zdn

dσ2

dt= 2α′1,0(φ)σ2 + α2,0(φ)

Carl Boettiger, UC Davis Biological Fluctuations 7/21

Page 8: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Near Equilibrium: Fluctuation Dissipation Regime

In the dissipation regime, fluctuations exponentially relax to theequilibrium level

σ2 = b(n)+d(n)2[d′(n)−b′(n)]

N = 1000, e = 0.2,c = 1

n = Nˆ1− e

c

˜= 800

σ2 = N ec

= 200

Dots are simulationaverages, lines aretheoretical prediction

Carl Boettiger, UC Davis Biological Fluctuations 8/21

Page 9: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Fluctuation Enhancement

With an initial condition starting deep in the enhancement regime,fluctuations grow exponentially. At N = 400, dissipation takes overand fluctuations return to the same equilibrium as before.

Carl Boettiger, UC Davis Biological Fluctuations 9/21

Page 10: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

1 Noisy Biology

2 Fluctuation Regimes

3 Model Choice

4 Macroscopic Phenomena

5 Fluctuation Dominance

Carl Boettiger, UC Davis Biological Fluctuations 10/21

Page 11: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Which model best describes this data?

dn

dt= c

n

N

“1− n

N

”| z

bn

− en

N|zdn

dn

dt= rn|z

bn

− rn2

K|zdn

. . . and why does it matter?

Carl Boettiger, UC Davis Biological Fluctuations 11/21

Page 12: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Using the Information Hidden in the Fluctuations

1 Independently parameterizebirth & death rates, see which isdensity dependent

2 Works with single realization atequilibrium

3 With replicates: The dynamicequations can determinefunctions b(n) and d(n)

4 Uses more information to informmodel choice

5 Can discount weights of pointsfrom high-variance regions whenmodel-fitting

Predicted fluctuations

Carl Boettiger, UC Davis Biological Fluctuations 12/21

Page 13: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

1 Noisy Biology

2 Fluctuation Regimes

3 Model Choice

4 Macroscopic Phenomena

5 Fluctuation Dominance

Carl Boettiger, UC Davis Biological Fluctuations 13/21

Page 14: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Stochastic Corrections: Deflation and Inflation

α′′1,0(φ) < 0 =⇒ Fluctuations

suppress the average relative tothe deterministic approximation.

Our theory accurately predictsthe extent of this effect.

Recall α2,0 = bn + dn controlsthe magnitude of this effect.

Ecological and evolutionaryconsequences for whenvariability is favorable?

dφdt

= α1,0(φ)+α′′1,0(φ)σ2

Carl Boettiger, UC Davis Biological Fluctuations 14/21

Page 15: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Fluctuation Phenomena: Deflation

dn

dt= c

n

N

“1− n

N

”| z

bn

− en

N|zdn

dt= α1,0(φ)+α′′1,0(φ)σ2

Carl Boettiger, UC Davis Biological Fluctuations 15/21

Page 16: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

1 Noisy Biology

2 Fluctuation Regimes

3 Model Choice

4 Macroscopic Phenomena

5 Fluctuation Dominance

Carl Boettiger, UC Davis Biological Fluctuations 16/21

Page 17: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Fluctuation Dominance

Far from equilibrium, enhancement can expand the fluctuationsuntil they reach the macroscopic scale.

Variance equation fails dramatically

Mean trajectory need not follow the deterministic trajectory

Bimodal distribution of trajectories can emerge

Conjecture: occurs when neighborhood exists for whichα1,0 ≈ 0 and α′

1,0 ≈ 0

Carl Boettiger, UC Davis Biological Fluctuations 17/21

Page 18: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Breakdown of the approximation

Carl Boettiger, UC Davis Biological Fluctuations 18/21

Page 19: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Breakdown of the Canonical Equation of AdaptiveDynamics

Carl Boettiger, UC Davis Biological Fluctuations 19/21

Page 20: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Further Topics

This approach can be applied to a variety of stochastic processes inbiology. . .

The multivariate theory: multiple species or age structuredpopulations. Predicts covariances as well.

Macroevolutionary theory: inferring speciation andextinction rates from phylogenetic trees

Adaptive dynamics: quantifying uncertainty in the canonicalequation, correcting for fluctuations.

Carl Boettiger, UC Davis Biological Fluctuations 20/21

Page 21: Reading the Secrets of Biological Fluctuations

Noisy Biology Fluctuation Regimes Model Choice Macroscopic Phenomena Fluctuation Dominance

Acknowledgments

Advisors & Advice

Alan HastingsJoshua WeitzMany here for helpfuldiscussions!

Funding

DOE CSGFUC Davis PopulationBiology Graduate Group

Carl Boettiger, UC Davis Biological Fluctuations 21/21