Heat conduction in a chain of colliding particles with stiff repulsive potential
O.V. Gendelman, A.V. Savin

TL;DR
This paper studies heat conduction in a chain of particles with finite interaction time, revealing saturation of heat conduction coefficient and an inverse relation to particle density, supported by simulations.
Contribution
It introduces a model with finite-time collisions in a particle chain, showing non-integrability, heat conduction saturation, and a simple kinetic description of heat transport.
Findings
Heat conduction coefficient saturates for large system sizes.
The inverse proportionality of HCC to particle density.
Validation of predictions through numerical simulations.
Abstract
One-dimensional billiard, i.e. a chain of colliding particles with equal masses, is well-known example of completely integrable system. Billiards with different particles are generically not integrable, but still exhibit divergence of a heat conduction coefficient (HCC) in thermodynamic limit. Traditional billiard models imply instantaneous (zero-time) collisions between the particles. We lift this condition and consider the heat transport in a chain of stiff colliding particles with power-law potential of the nearest-neighbor interaction. The instantaneous collisions correspond to the limit of infinite power in the interaction potential; for finite powers, the interactions take nonzero time. This modification of the model leads to profound physical consequence -- probability of multiple, in particular, triple particle collisions becomes nonzero. Contrary to the integrable billiard of…
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