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Heat Transport of the ββ-Fermi--Pasta--Ulam--Tsingou chain in the long-wave limit

Published 7 Oct 2026 in cond-mat.stat-mech, physics.class-ph, physics.comp-ph, and physics.pop-ph | (2610.09405v1)

Abstract: Resolving the anomalous conductivity exponent of the symmetric ββ-Fermi--Pasta--Ulam--Tsingou chain by molecular dynamics can require very large systems because of long finite-size crossovers and thermal-contact resistance. Motivated by this computational challenge, we derive a long-wavelength continuum description and investigate whether the kinetic-theory scaling κ∝L<sup>2/5κ\propto L<sup>{2/5} becomes accessible with a moderate number of numerical degrees of freedom. The nonlinear elastic field retains the cubic stress of the microscopic interaction and exchanges heat with Langevin reservoirs. A flux-conservative spatial discretization constructs the force and energy current from the same stress, providing a consistent interior transport estimator. For $L&gt;8$, corresponding to approximately $103$ mesh nodes and above at the reference resolution, the fitted exponent is 0.399±0.0040.399\pm0.004. Mesh refinement supports the stability of this exponent between the two finer resolutions, although the conductivity amplitude remains resolution-dependent. The main result is thus an accessible finite-size regime near $2/5$, rather than convergence of the absolute conductivity as the mesh spacing vanishes. This formulation provides a practical route to studying anomalous transport in anharmonic systems and a conservative continuum framework for investigating energy flow in nonlinear elastic media.

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