4.6 Article

First-principle validation of Fourier's law in d=1, 2, 3 classical systems

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PHYSICA D-NONLINEAR PHENOMENA
卷 446, 期 -, 页码 -

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ELSEVIER
DOI: 10.1016/j.physd.2023.133681

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Nonextensive statistical mechanics; Langevin dynamics; Linear transport phenomena; Irreversibility

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This paper numerically studies the thermal transport in d=1,2,3 dimensions of classical inertial nearest-neighbor XY ferromagnet. The expression of thermal conductance is found to be related to the system size L and temperature T, and inversely proportional to the thermal conductance in the infinite system size limit. These findings contribute to the understanding of the thermal conductivity of materials.
We numerically study the thermal transport in the classical inertial nearest-neighbor XY ferromagnet in d = 1, 2, 3, the total number of sites being given by N = Ld, where L is the linear size of the system. For the thermal conductance sigma, we obtain sigma(T, L)L delta(d)= A(d) e-B(d) [L gamma (d)T ]eta(d) (with ez q(d) q equivalent to [1+(1-q)z]1/(1-q); ez1 = ez; A(d) > 0; B(d) > 0; q(d) > 1; eta(d) > 2; delta >= 0; gamma(d) > 0), for all values of L gamma(d)T for d = 1, 2, 3. In the L -> infinity limit, we have sigma proportional to 1/L rho sigma(d) with rho sigma(d) = delta(d)+gamma(d)eta(d)/[q(d)-1]. The material conductivity is given by kappa = sigma Ld proportional to 1/L rho kappa(d) (L -> infinity) with rho kappa(d) = rho sigma(d) - d. Our numerical results are consistent with 'conspiratory' d-dependences of (q, eta, delta, gamma), which comply with normal thermal conductivity (Fourier law) for all dimensions.(c) 2023 Published by Elsevier B.V.

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