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  • Letter
  • Open Access

Generalized Fourier’s law in mesoscopic systems

Luciano C. Lapas*

  • *Contact author: luciano.lapas@unila.edu.br

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 κeff(k,ω), 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 Λz≠Λr. 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 0.25–0.4μm. 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 Si0.2Ge0.8, and the rise of the apparent interface conductance of Al/Si0.99Ge0.01, and contains the two-channel ballistic/diffusive model as a two-sector projection.

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References (57)

  1. G. Chen, Nanoscale Energy Transport and Conversion: A Parallel Treatment of Electrons, Molecules, Phonons, and Photons (Oxford University Press, New York, 2005).
  2. J.-J. Greffet, Electrons and phonons, in Microscale and Nanoscale Heat Transfer, edited by S. Volz (Springer, Berlin, 2007), pp. 37–54.
  3. J. B. J. Fourier, Théorie Analytique de la Chaleur (Didot, Paris, 1822).
  4. J.-J. Greffet, Laws of macroscopic heat transfer and their limits, in Microscale and Nanoscale Heat Transfer, edited by S. Volz (Springer, Berlin, 2007), pp. 1–13.
  5. D. Bimberg, M. Grundmann, and N. N. Ledentsov, Quantum Dot Heterostructures (John Wiley & Sons, Chichester, 1999).
  6. B. J. Berne and R. Pecora, Dynamic Light Scattering: With Applications to Chemistry, Biology, and Physics (Dover, New York, 2000).
  7. B. Alberts, R. Heald, A. Johnson, D. Morgan, M. C. Raff, K. Roberts, and P. Walter, Molecular Biology of the Cell (W. W. Norton & Company, New York, 2022).
  8. D. G. Cahill, W. K. Ford, K. E. Goodson, G. D. Mahan, A. Majumdar, H. J. Maris, R. Merlin, and S. R. Phillpot, Nanoscale thermal transport, J. Appl. Phys. 93, 793 (2003).
  9. J. A. Johnson, A. A. Maznev, J. Cuffe, J. K. Eliason, A. J. Minnich, T. Kehoe, C. M. Torres, G. Chen, and K. A. Nelson, Direct measurement of room-temperature nondiffusive thermal transport over micron distances in a silicon membrane, Phys. Rev. Lett. 110, 025901 (2013).
  10. R. B. Wilson and D. G. Cahill, Anisotropic failure of Fourier theory in time-domain thermoreflectance experiments, Nat. Commun. 5, 5075 (2014).
  11. K. Zheng, S. Ghosh, and S. Granick, Exceptions to Fourier’s law at the macroscale, Proc. Natl. Acad. Sci. USA 121, e2320337121 (2024).
  12. A. A. Maznev, J. A. Johnson, and K. A. Nelson, Onset of nondiffusive phonon transport in transient thermal grating decay, Phys. Rev. B 84, 195206 (2011).
  13. J. P. Feser and D. G. Cahill, Probing anisotropic heat transport using time-domain thermoreflectance with offset laser spots, Rev. Sci. Instrum. 83, 104901 (2012).
  14. G. D. Mahan and F. Claro, Nonlocal theory of thermal conductivity, Phys. Rev. B 38, 1963 (1988).
  15. Y. K. Koh, D. G. Cahill, and B. Sun, Nonlocal theory for heat transport at high frequencies, Phys. Rev. B 90, 205412 (2014).
  16. C. Hua and A. J. Minnich, Analytical Green’s function of the multidimensional frequency-dependent phonon Boltzmann equation, Phys. Rev. B 90, 214306 (2014).
  17. P. B. Allen and V. Perebeinos, Temperature in a Peierls-Boltzmann treatment of nonlocal phonon heat transport, Phys. Rev. B 98, 085427 (2018).
  18. C. Hua and L. Lindsay, Space-time dependent thermal conductivity in nonlocal thermal transport, Phys. Rev. B 102, 104310 (2020).
  19. F. Yang and C. Dames, Heating-frequency-dependent thermal conductivity: An analytical solution from diffusive to ballistic regime and its relevance to phonon scattering measurements, Phys. Rev. B 91, 165311 (2015).
  20. A. J. Minnich, J. A. Johnson, A. J. Schmidt, K. Esfarjani, M. S. Dresselhaus, K. A. Nelson, and G. Chen, Thermal conductivity spectroscopy technique to measure phonon mean free paths, Phys. Rev. Lett. 107, 095901 (2011).
  21. D. Ding, X. Chen, and A. J. Minnich, Radial quasiballistic transport in time-domain thermoreflectance studied using Monte Carlo simulations, Appl. Phys. Lett. 104, 143104 (2014).
  22. C. Hua, L. Lindsay, X. Chen, and A. J. Minnich, Generalized Fourier’s law for nondiffusive thermal transport: Theory and experiment, Phys. Rev. B 100, 085203 (2019).
  23. A. Beardo, S. Alajlouni, L. Sendra, J. Bafaluy, A. Ziabari, Y. Xuan, J. Camacho, A. Shakouri, and F. X. Alvarez, Hydrodynamic thermal transport in silicon at temperatures ranging from 100 to 300 K, Phys. Rev. B 105, 165303 (2022).
  24. Z. Xiang, P. Jiang, and R. Yang, Time-domain thermoreflectance (TDTR) data analysis using phonon hydrodynamic model, J. Appl. Phys. 132, 205104 (2022).
  25. R. B. Wilson, J. P. Feser, G. T. Hohensee, and D. G. Cahill, Two-channel model for nonequilibrium thermal transport in pump-probe experiments, Phys. Rev. B 88, 144305 (2013).
  26. Y. Zeng and J. Dong, Unified statistical theory of heat conduction in nonuniform media, Phys. Rev. B 113, 235204 (2026).
  27. See Supplemental Material at http://link.aps.org/supplemental/10.1103/ggz5-nggb for the derivation of the constitutive law, the generalized Langevin equation and the modal Onsager kernel, its relaxation-time closure and tensor structure, the through-plane boundary-value problem and the interfacial nonequilibrium resistance, the mean-free-path spectra and thermoreflectance forward model, the fitting procedure and uncertainties, a comparison with previous treatments, and testable predictions, which includes Refs. [28, 29, 30, 31, 32, 33, 34].
  28. L. Onsager, Reciprocal relations in irreversible processes. I, Phys. Rev. 37, 405 (1931).
  29. L. Onsager, Reciprocal relations in irreversible processes. II, Phys. Rev. 38, 2265 (1931).
  30. K. Esfarjani, G. Chen, and H. T. Stokes, Heat transport in silicon from first-principles calculations, Phys. Rev. B 84, 085204 (2011).
  31. K. T. Regner, D. P. Sellan, Z. Su, C. H. Amon, A. J. H. McGaughey, and J. A. Malen, Broadband phonon mean free path contributions to thermal conductivity measured using frequency domain thermoreflectance, Nat. Commun. 4, 1640 (2013).
  32. S.-I. Tamura, Isotope scattering of dispersive phonons in Ge, Phys. Rev. B 27, 858 (1983).
  33. J. Carrete, B. Vermeersch, A. Katre, A. van Roekeghem, T. Wang, G. K. H. Madsen, and N. Mingo, almaBTE: A solver of the space–time dependent Boltzmann transport equation for phonons in structured materials, Comput. Phys. Commun. 220, 351 (2017).
  34. B. Vermeersch, J. Carrete, N. Mingo, and A. Shakouri, Superdiffusive heat conduction in semiconductor alloys. I. Theoretical foundations, Phys. Rev. B 91, 085202 (2015).
  35. S. R. de Groot and P. Mazur, Non-Equilibrium Thermodynamics (Dover, New York, 1984).
  36. J. M. G. Vilar and J. M. Rubí, Thermodynamics “beyond” local equilibrium, Proc. Natl. Acad. Sci. USA 98, 11081 (2001).
  37. D. Reguera, J. M. Rubí, and J. M. G. Vilar, The mesoscopic dynamics of thermodynamic systems, J. Phys. Chem. B 109, 21502 (2005).
  38. H. Mori, Transport, collective motion, and Brownian motion, Prog. Theor. Phys. 33, 423 (1965).
  39. R. Kubo, Statistical-mechanical theory of irreversible processes. I. General theory and simple applications to magnetic and conduction problems, J. Phys. Soc. Jpn. 12, 570 (1957).
  40. R. Zwanzig, Memory effects in irreversible thermodynamics, Phys. Rev. 124, 983 (1961).
  41. R. Zwanzig, Nonequilibrium Statistical Mechanics (Oxford University Press, New York, 2001).
  42. B. H. Armstrong, Two-fluid theory of thermal conductivity of dielectric crystals, Phys. Rev. B 23, 883 (1981).
  43. L. Zhu, A. Fiorino, D. Thompson, R. Mittapally, E. Meyhofer, and P. Reddy, Near-field photonic cooling through control of the chemical potential of photons, Nature (London) 566, 239 (2019).
  44. K. Chen and S. Fan, Nonequilibrium Casimir force with a nonzero chemical potential for photons, Phys. Rev. Lett. 117, 267401 (2016).
  45. D. G. Cahill, Analysis of heat flow in layered structures for time-domain thermoreflectance, Rev. Sci. Instrum. 75, 5119 (2004).
  46. K. Schwab, E. A. Henriksen, J. M. Worlock, and M. L. Roukes, Measurement of the quantum of thermal conductance, Nature (London) 404, 974 (2000).
  47. R. Morgado, F. A. Oliveira, G. G. Batrouni, and A. Hansen, Relation between anomalous and normal diffusion in systems with memory, Phys. Rev. Lett. 89, 100601 (2002).
  48. L. C. Lapas, I. V. L. Costa, M. H. Vainstein, and F. A. Oliveira, Entropy, non-ergodicity and non-Gaussian behaviour in ballistic transport, Europhys. Lett. 77, 37004 (2007).
  49. M. H. Vainstein, I. V. L. Costa, R. Morgado, and F. A. Oliveira, Non-exponential relaxation for anomalous diffusion, Europhys. Lett. 73, 726 (2006).
  50. L. C. Lapas, R. Morgado, M. H. Vainstein, J. M. Rubí, and F. A. Oliveira, Khinchin theorem and anomalous diffusion, Phys. Rev. Lett. 101, 230602 (2008).
  51. E. G. Flekkøy, A. Hansen, and B. Baldelli, Hyperballistic superdiffusion and explosive solutions to the non-linear diffusion equation, Front. Phys. 9, 640560 (2021).
  52. C. Cattaneo, Sulla conduzione del calore, Atti Semin. Mat. Fis. Univ. Modena 3, 83 (1948).
  53. P. Vernotte, La véritable équation de la chaleur, C. R. Hebd. Séances Acad. Sci. 247, 2103 (1958).
  54. R. A. Guyer and J. A. Krumhansl, Thermal conductivity, second sound, and phonon hydrodynamic phenomena in nonmetallic crystals, Phys. Rev. 148, 778 (1966).
  55. Y. K. Koh and D. G. Cahill, Frequency dependence of the thermal conductivity of semiconductor alloys, Phys. Rev. B 76, 075207 (2007).
  56. A. J. Minnich, Advances in the measurement and computation of thermal phonon transport properties, J. Phys.: Condens. Matter 27, 053202 (2015).
  57. M. S. Gomes-Filho, L. C. Lapas, E. Gudowska-Nowak, and F. A. Oliveira, The fluctuation–dissipation relations: Growth, diffusion, and beyond, Phys. Rep. 1141, 1 (2025).

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