Abstract

Motivated by the collective behavior of biological swarms, we study the critical dynamics of field theories with coupling between order parameter and conjugate momentum in the presence of dissipation. Under a fixed-network approximation, we perform a dynamical renormalization group calculation at one loop in the near-critical disordered region, and we show that the violation of momentum conservation generates a crossover between an unstable fixed point, characterized by a dynamic critical exponent z=d/2, and a stable fixed point with z=2. Interestingly, the two fixed points have different upper critical dimensions. The interplay between these two fixed points gives rise to a crossover in the critical dynamics of the system, characterized by a crossover exponent κ=4/d. The crossover is regulated by a conservation length scale R_{0}, given by the ratio between the transport coefficient and the effective friction, which is larger as the dissipation is smaller: Beyond R_{0}, the stable fixed point dominates, while at shorter distances dynamics is ruled by the unstable fixed point and critical exponent, a behavior which is all the more relevant in finite-size systems with weak dissipation. We run numerical simulations in three dimensions and find a crossover between the exponents z=3/2 and z=2 in the critical slowdown of the system, confirming the renormalization group results. From the biophysical point of view, our calculation indicates that in finite-size biological groups mode coupling terms in the equation of motion can significantly change the dynamical critical exponents even in the presence of dissipation, a step toward reconciling theory with experiments in natural swarms. Moreover, our result provides the scale within which fully conservative Bose-Einstein condensation is a good approximation in systems with weak symmetry-breaking terms violating number conservation, as quantum magnets or photon gases.

Highlights

  • The success of the theory of critical phenomena is based upon a simple observation: Systems with very different microscopic details behave in strikingly similar ways when correlations are sufficiently strong

  • We perform a dynamical renormalization group calculation at one loop in the nearcritical disordered region, and we show that the violation of momentum conservation generates a crossover between an unstable fixed point, characterized by a dynamic critical exponent z = d/2, and a stable fixed point with z = 2

  • Where we emphasize that all integrals that appear in the right-hand side through the factor δPl must be evaluated at the running value of the parameters, namely at their value at the renormalization group (RG) step l, whereas the naive physical dimension DP is fixed once and for all

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Summary

INTRODUCTION

The success of the theory of critical phenomena is based upon a simple observation: Systems with very different microscopic details behave in strikingly similar ways when correlations are sufficiently strong. We have theories ruled by symmetry and conservation laws, whose dynamics is characterized by the coupling between two fields, namely the order parameter and the conserved generator of the symmetry, i.e., the conjugate momentum This second type of theories has nondissipative mode-coupling terms in the equations of motion and was originally introduced to describe systems displaying Bose-Einstein condensation (BEC), as superfluid helium, superconductivity, and quantum magnets A shorter account of our results can be found in Ref. [32]

BIOPHYSICAL ORIGIN OF THE MICROSCOPIC MODEL
Collective behavior and the Vicsek model
The inertial spin model
Fixed network approximation
Equations of motion
Free theory in Fourier space
RENORMALIZATION GROUP IN MOMENTUM SHELL
Integration of the short-wavelength details
Rescaling of space and time
Renormalization group recursive equations
Fixed points and dynamic critical exponent
The IR-unstable conservative fixed point
The IR-stable dissipative fixed point
RG flow on the critical manifold
Crossover in the critical dynamics
A new upper critical dimension
CALLAN-SYMANZIK APPROACH
Renormalized theory and renormalization factors
RG equation and dynamic critical exponent
Determination of Z factors
Determination of the crossover factor X
Fixed points
Crossover
NUMERICAL SIMULATIONS
Static behavior and determination of ξ
Dynamic behavior and determination of τ
Dynamic crossover
Natural swarms and inertial dynamics
VIII. CONCLUSIONS
Martin-Siggia-Rose formalism
Perturbation expansion at one loop
Full Text
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