Abstract
Considering a system of N identical interacting particles, which obey Fermi-Dirac or Bose-Einstein statistics, we derive new formulas for correlation functions of the type {Mathematical expression} (where Bj is diagonal in the free-particle states) in the thermodynamic limit. Thereby we apply and extend a superoperator formalism, recently developed for the derivation of long-time tails in semiclassical systems. As an illustrative application, the Boltzmann equation value of the time-integrated correlation function C(t) is derived in a straightforward manner. Due to exchange effects, the obtained t-matrix and the resulting scattering cross section, which occurs in the Boltzmann collision operator, are now functionals of the Fermi-Dirac or Bose-Einstein distribution.
| Original language | English |
|---|---|
| Pages (from-to) | 765-795 |
| Number of pages | 31 |
| Journal | Journal of Statistical Physics |
| Volume | 54 |
| Issue number | 3-4 |
| DOIs | |
| State | Published - Feb 1989 |
Keywords
- cluster expansion
- exchange effects
- Liouville operators
- Time correlation functions
ASJC Scopus subject areas
- Statistical and Nonlinear Physics
- Mathematical Physics
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