We present an effective field theory for the nonlinear fluctuating hydrodynamics of a single conserved charge with or without time-reversal symmetry, based on the Martin-Siggia-Rose formalism. Applying this formalism to fluids with only charge and multipole conservation, and with broken time-reversal symmetry, we predict infinitely many new dynamical universality classes, including some with arbitrarily large upper critical dimensions. Using large scale simulations of classical Markov chains, we find numerical evidence for a breakdown of hydrodynamics in quadrupole-conserving models with broken time-reversal symmetry in one spatial dimension.Comment: 5+3 pages; 1+1 figure
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When continuous rotational invariance of a two-dimensional fluid is broken to the discrete, dihedral...
We consider fermions defined on a continuous one-dimensional interval and subject to weak repulsive ...
We show how causal relativistic Navier-Stokes equations arise from the relativistic Boltzmann equati...
We investigate the coupled dynamics of charge and energy in interacting lattice models with dipole c...
We study charged hydrodynamics in a periodic lattice background. Fluctuations are Bloch waves rather...
The article by M. Waclawczyk et al. [Phys. Rev. E 90, 013022 (2014)] proposes two new statistical sy...
We examine the role discrete symmetries, time-reversal and mirror symmetries, play in the context of...
We study the quasi-hydrodynamics of a system with a softly broken $U(1)$ global symmetry using effec...
We propose a general hydrodynamic framework for systems with spontaneously broken approximate symmet...
We argue that different formulations of hydrodynamics are related to uncertainties in the definition...
International audienceWe derive a dynamical equation that describes the exact time evolution in gene...
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