Abstract

A unified set of hydrodynamic equations describing condensed phases of matter with broken continuous symmetries is derived using a generalization of the statistical-mechanical approach based on the local equilibrium distribution. The dissipativeless and dissipative parts of the current densities and the entropy production are systematically deduced in this approach by expanding in powers of the gradients of the macrofields. Green–Kubo formulas are obtained for all the linear transport coefficients. The consequences of microreversibility and spatial symmetries are investigated, leading to the prediction of cross effects resulting from Onsager–Casimir reciprocal relations. Crystalline solids and liquid crystals are potential examples of application. The approach is clarifying the links between the microscopic Hamiltonian dynamics and the thermodynamic and transport properties at the macroscale.

Highlights

  • A unified set of hydrodynamic equations describing condensed phases of matter with broken continuous symmetries is derived using a generalization of the statistical-mechanical approach based on the local equilibrium distribution

  • In nematic liquid crystals, the part of the Hamiltonian ruling the rotation of the system around the orientation selected by spontaneous symmetry breaking should be separated from the rest of the Hamiltonian function in order to define equilibrium probability distributions describing the properties of the phase with broken symmetry

  • We have shown that the macroscopic equations ruling the time evolution of matter with broken continuous symmetries can be derived in a unified microscopic approach based on the local equilibrium distribution, extending to crystalline solids and liquid crystals results previously obtained for normal fluids

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Summary

Introduction

The spontaneous breaking of continuous symmetries is a ubiquitous phenomenon in nature. Microscopic approach to the macrodynamics of matter with broken symmetries has been developed since the sixties [25,26,27,28,29,30,31,32,33,34,35], provides the microscopic expressions for the dissipativeless fluxes of Eulerian type, and local thermodynamics and the statistical-mechanical expression for entropy production in terms of the dissipative fluxes These latter fluxes can be obtained at leading order in the gradients of the macrofields together with the transport coefficients given by Green–Kubo formulas. Einstein’s convention of summation over repeated indices is adopted

Hamiltonian dynamics
Conserved quantities
Breaking of continuous symmetries
Nambu–Goldstone modes
Nonequilibrium statistical mechanics
Time evolution
Local equilibrium distribution
Time evolution of the local equilibrium distribution
Entropy production and dissipative current densities
Local thermodynamics
The conjugated fields
Gibbs–Duhem relation and consequences
Dissipativeless current densities
Galilean transformations
Dissipativeless current densities of energy and momentum
Dissipativeless local conservation equations
Dissipativeless equations for the conjugated fields
Dissipative current densities
Heat current density
Deduction at leading order
Green–Kubo formulas for the transport coefficients
Time-reversal symmetry
Entropy production
Macroscopic equations
Crystalline solids
Order parameters
Green–Kubo formulas
Liquid crystals
Conclusion
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