Article Outline
Glossary
Definition of the Subject
Introduction
Weak‐Coupling Limit for Classical Systems
Weak‐Coupling Limit for Quantum Systems
Weak-Coupling Limit in the Bose–Einstein and Fermi–Dirac Statistics
Weak-Coupling Limit for a Single Particle: The Linear Theory
Future Directions
Bibliography
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Abbreviations
- Scaling limits:
-
A scaling limit denotes a procedure to reduce the degree of complexity of a large particle system. It consists in scaling the space-time variables and, possibly, other quantities (like the interaction potential or the density), in order to obtain a more handable description of the same system. The initial space-time coordinates are called microscopic, while the new ones, those well suited for the description of kinetic or hydrodynamical systems, are called macroscopic.
- Boltzmann equation:
-
It is an integro‐differential kinetic equation for the one particle distribution function in the classical phase space (see Eq. (64) below). It arises in some physical regimes, namely for a rarefied gas and for a weakly interacting quantum dense gas.
- Uehling–Uhlenbeck equation:
-
It is a Boltzmann type equation taking into account corrections due to the Bose–Einstein or the Fermi–Dirac statistics (see Eq. (69) below). It holds in the weak‐coupling limit.
- Fokker–Planck–Landau equation:
-
It is a kinetic equation diffusive in velocity (see Eq. (28) below). It arises in the context of a weakly interacting classical dense gas.
- Hydrodynamical equations:
-
They are evolution equations for macroscopic quantities like density, mean velocity, temperature, and so on.
- Low density limit:
-
Sometimes called Boltzmann–Grad limit, it is a scaling limit in which the density is vanishing. Applied to classical particle systems it gives the Boltzmann equation.
- Weak coupling limit:
-
It is a scaling limit in which the density is constant but the interaction vanishes suitably. Applied to a quantum particle systems it gives a Boltzmann equation. Applied to a classical particle systems it gives the Fokker–Planck–Landau equation.
- Hydrodynamic limit:
-
In this scaling we simply pass from micro to macro variables. We look at the behavior of suitable mean values, which are functions of the space and the time. We expect them to behave in a hydrodynamical way, namely to satisfy a set of hydrodynamical equations.
- Wigner transform:
-
It is the description of a quantum state as a function in the classical phase space.
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Benedetto, D., Pulvirenti, M. (2012). Scaling Limits of Large Systems of Non-linear Partial Differential Equations. In: Meyers, R. (eds) Mathematics of Complexity and Dynamical Systems. Springer, New York, NY. https://doi.org/10.1007/978-1-4614-1806-1_95
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