Quantum ideal hydrodynamics on the lattice
arXiv:1311.3333
Abstract
After discussing the problem of defining the hydrodynamic limit from microscopic scales, we give an introduction to ideal hydrodynamics in the Lagrange picture, and show that it can be viewed as a field theory, which can be quantized using the usual Feynman sum-over-paths prescription. We then argue that this picture can be connected to the usually neglected thermal microscopic scale in the hydrodynamic expansion. After showing that this expansion is generally non-perturbative, we show how the lattice can be used to understand the impact quantum and thermal fluctuations can have on the fluid behavior.
References in corpus (5)
- Viscosity in Strongly Interacting Quantum Field Theories from Black Hole Physics
- Effective field theory for hydrodynamics: thermodynamics, and the derivative expansion
- The stickiness of sound: An absolute lower limit on viscosity and the breakdown of second order relativistic hydrodynamics
- The quantum mechanics of perfect fluids
- Viscosity of an ideal relativistic quantum fluid: A perturbative study