- Letter
- Open Access
Generalized Fourier’s law in mesoscopic systems
APS Open Sci. 1, L000216 – Published 13 November, 2026
DOI: https://doi.org/10.1103/ggz5-nggb
Abstract
Fourier’s law fails when the mean free path of the energy carriers becomes comparable to the length scales and timescales over which the temperature field varies. We derive a thermodynamically consistent generalization in which the conductivity becomes a nonlocal memory operator , by combining mesoscopic nonequilibrium thermodynamics with the Mori-Kubo–Zwanzig projection-operator formalism. The Onsager kernel is a tensor sum over vibrational normal modes weighted by their Bose heat capacities and relaxation functions; it satisfies the second law for any closure consistent with the fluctuation-dissipation theorem and reduces, in the relaxation-time closure, to the nonlocal conductivity of the phonon Boltzmann equation. Two consequences follow. First, direction-dependent sampling of this tensor in a pump-probe experiment makes a nominally isotropic crystal exhibit apparent conductivities . Second, the modulation frequency does not introduce temporal memory but sets the probed wave vector through the thermal penetration depth, so that the frequency-dependent suppression of the apparent conductivity measured by time-domain thermoreflectance on Ge and SiGe alloys is a spatial-nonlocality effect, with effective lengths of . With published mean-free-path spectra and no parameter adjusted to the thermoreflectance data, the kernel reproduces the spot-size dependence of Si, the frequency dependence of the apparent conductivity of Ge and , and the rise of the apparent interface conductance of , and contains the two-channel ballistic/diffusive model as a two-sector projection.
Physics Subject Headings (PhySH)
Article Text
Supplemental Material
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