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PreprintCC BY 4.0arXiv

Heat transport in weakly anharmonic Fermi-Pasta-Ulam-Tsingou chains

Abstract

We investigate anomalous heat transport in the one-dimensional β-Fermi--Pasta--Ulam--Tsingou chain in the weakly anharmonic regime using large-scale equilibrium molecular dynamics. By resolving the heat current into phonon-mode contributions, we show that its long-time autocorrelation is controlled by diagonal mode correlations, whose decay is quantitatively determined by the corresponding phonon damping rates. Extrapolation to the thermodynamic limit gives Γk ∝ (βT)4/3 k5/3, with a subleading k2 correction. The latter produces an extended pre-asymptotic regime, C(t) ∼ t−4/5, before the asymptotic decay C(t) ∼ t−3/5 is reached, leading to κ(N) ∼ N2/5 + O(N1/5). At weak anharmonicity, off-diagonal mode correlations persist up to a characteristic time τod ∼ (βT)−2, while increasingly large systems are required to resolve the long-wavelength phonon contribution. Weak anharmonicity therefore does not introduce a distinct asymptotic transport mechanism, but shifts the onset of the phonon-dominated regime to progressively longer times and larger length scales.

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BibTeX
@misc{sharma2026heat,
  title = {{Heat transport in weakly anharmonic Fermi-Pasta-Ulam-Tsingou chains}},
  author = {Kiratholly Nandakumar Madhav Sharma and Stefano Mossa and Jean-Louis Barrat and Markus Holzmann},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.09936},
  eprint = {2610.09936},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.09936},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Heat transport in weakly anharmonic Fermi-Pasta-Ulam-Tsingou chains
AU  - Kiratholly Nandakumar Madhav Sharma
AU  - Stefano Mossa
AU  - Jean-Louis Barrat
AU  - Markus Holzmann
PY  - 2026
DA  - 2026/10/07
PB  - arXiv
DO  - 10.48550/arxiv.2610.09936
UR  - https://arxiv.org/abs/2610.09936
AB  - We investigate anomalous heat transport in the one-dimensional β-Fermi--Pasta--Ulam--Tsingou chain in the weakly anharmonic regime using large-scale equilibrium molecular dynamics. By resolving the heat current into phonon-mode contributions, we show that its long-time autocorrelation is controlled by diagonal mode correlations, whose decay is quantitatively determined by the corresponding phonon damping rates. Extrapolation to the thermodynamic limit gives Γ_k ∝ (βT)^4/3 k^5/3, with a subleading k^2 correction. The latter produces an extended pre-asymptotic regime, C(t) ∼ t^−4/5, before the asymptotic decay C(t) ∼ t^−3/5 is reached, leading to κ(N) ∼ N^2/5 + O(N^1/5). At weak anharmonicity, off-diagonal mode correlations persist up to a characteristic time τ_od ∼ (βT)^−2, while increasingly large systems are required to resolve the long-wavelength phonon contribution. Weak anharmonicity therefore does not introduce a distinct asymptotic transport mechanism, but shifts the onset of the phonon-dominated regime to progressively longer times and larger length scales.
ER  -