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On the asymptotic behavior at the kinetic time of a weakly interacting Fermi gas

Abstract

This paper is devoted to the dynamics of a weakly interacting Fermi gas at the kinetic time regime t∼ λ−2 where λ≪ 1 is the strength of the interaction potential. We prove that if the initial state is close to equilibrium, then the two-point time correlation function of the many-body quantum dynamics can be computed effectively. In fact, we show that its leading order behavior is determined completely by the collisional frequency of the Boltzmann-Nordheim collision operator at equilibrium. This settles a prediction by Lukkarinen-Spohn, and thus gives a justification of the quantum Boltzmann equation from many-body quantum mechanics.

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BibTeX
@misc{madsen2026asymptotic,
  title = {{On the asymptotic behavior at the kinetic time of a weakly interacting Fermi gas}},
  author = {Peter S. Madsen and Phan Thành Nam and Herbert Spohn and Minh-Binh Tran},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2605.13499},
  eprint = {2605.13499},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2605.13499},
}
RIS
TY  - UNPB
TI  - On the asymptotic behavior at the kinetic time of a weakly interacting Fermi gas
AU  - Peter S. Madsen
AU  - Phan Thành Nam
AU  - Herbert Spohn
AU  - Minh-Binh Tran
PY  - 2026
DA  - 2026/11/02
PB  - arXiv
DO  - 10.48550/arxiv.2605.13499
UR  - https://arxiv.org/abs/2605.13499
AB  - This paper is devoted to the dynamics of a weakly interacting Fermi gas at the kinetic time regime t∼ λ^−2 where λ≪ 1 is the strength of the interaction potential. We prove that if the initial state is close to equilibrium, then the two-point time correlation function of the many-body quantum dynamics can be computed effectively. In fact, we show that its leading order behavior is determined completely by the collisional frequency of the Boltzmann-Nordheim collision operator at equilibrium. This settles a prediction by Lukkarinen-Spohn, and thus gives a justification of the quantum Boltzmann equation from many-body quantum mechanics.
ER  -