Abstract

We provide a complete solution to hydrodynamic transport at all orders in the gradient expansion compatible with the second law constraint. The key new ingredient we introduce is the notion of adiabaticity, which allows us to take hydrodynamics off-shell. Adiabatic fluids are such that off-shell dynamics of the fluid compensates for entropy production. The space of adiabatic fluids is quite rich, and admits a decomposition into seven distinct classes. Together with the dissipative class this establishes the eightfold way of hydrodynamic transport. Furthermore, recent results guarantee that dissipative terms beyond leading order in the gradient expansion are agnostic of the second law. While this completes a transport taxonomy, we go on to argue for a new symmetry principle, an Abelian gauge invariance that guarantees adiabaticity in hydrodynamics. We suggest that this symmetry is the macroscopic manifestation of the microscopic KMS invariance. We demonstrate its utility by explicitly constructing effective actions for adiabatic transport. The theory of adiabatic fluids, we speculate, provides a useful starting point for a new framework to describe non-equilibrium dynamics, wherein dissipative effects arise by Higgsing the Abelian symmetry.

Highlights

  • Hydrodynamics, as is well known, is the universal long-wavelength effective description of near-equilibrium dynamics of interacting quantum systems

  • While many attempts have been made to distill the essentials of the theory and derive the low energy dynamics following rules of effective field theory, it is perhaps fair to say that to date a completely autonomous theory of hydrodynamics remains in absentia

  • To motivate the study of adiabatic fluids, let us ask the following question: “what is the most convenient way to implement the second law of thermodynamics, which apriori is stated as an inequality, in practice?” As we discussed before the conventional current-algebraic approach is to work on-shell by classifying independent tensors, but this is limiting from the point of view of constructing an action principle

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Summary

Introduction

Hydrodynamics, as is well known, is the universal long-wavelength effective description of near-equilibrium dynamics of interacting quantum systems. To motivate the study of adiabatic fluids, let us ask the following question: “what is the most convenient way to implement the second law of thermodynamics, which apriori is stated as an inequality, in practice?” As we discussed before the conventional current-algebraic approach is to work on-shell by classifying independent tensors, but this is limiting from the point of view of constructing an action principle. This allows us to give an alternate proof of the theorem, classifying dissipative transport coefficients into those constrained by the second law, and those that are agnostic to entropy production. 12A clue to the existence of such a structure is provided by the analysis of hydrostatic partition functions satisfying the Euclidean consistency condition in the presence of gravitational anomalies [13]

§ 18: Discussion
Adiabatic hydrodynamics
The adiabaticity equation
Physical interpretation of adiabatic fluids
Ideal fluids are adiabatic
The adiabatic free energy current
Classification of adiabatic transport
T μν 2 gμν
Class H: hydrostatics from adiabaticity
Hydrostatic partition functions
Currents from the hydrostatic partition function
Class D: dissipative terms
Constraints on dissipative transport
Differential operators for dissipation
Examples: low order Class D differential operators
Class L
Bianchi identities in Class L
Noether current in Class L
T μν 2
Hydrostatic partition function for Class L
Hydrodynamic Ward identities in Class L
A constrained variational principle for hydrodynamics
Reference fields and conservation equations
Gauge redundancy of reference fields
Variational principle on reference manifold
Field redefinitions in Class L
Applications of adiabatic fluids
Class B
10 Class C: conserved entropy
11 The vector classes: transverse free energy currents
12 Class A: lagrangian solution to anomalous adiabaticity equation
13 Schwinger-Keldysh formalism for Class L and application to Class A
A A A δX
D D q u 1 b2 c
14 The eightfold way
15 Class LT: eightfold Lagrangian
16 Hydrodynamic Ward identities and the second law in Class LT
17 Eightfold adiabatic transport in Class LT
18 Discussion
19 Homework problems
Part V
Part VI
Relating variations of hydrodynamic fields to reference parameterization
Kσ σμα σαν
Background gauge field

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