Emergence of Nonlocal Hydrodynamics in Many-Body Radiative Heat Transport
Abstract
We develop a nonlocal hydrodynamic theory of radiative heat transport in many-body systems by coarse graining their microscopic electrodynamic interactions. Long-range radiative exchange naturally generates a spatially nonlocal constitutive relation in which the heat current at a given position depends on temperature gradients over an extended region, while energy conservation retains its local conservative form. Fourier transport emerges as a controlled long-wavelength limit when the interaction kernel has a finite second spatial moment. When this moment fails to converge, spatial nonlocality survives coarse graining and gives rise to non-Fourier transport. The resulting framework establishes a systematic bridge between discrete many-body fluctuational electrodynamics and a continuous description of radiative heat transport.
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BibTeX
@misc{viloria2026emergence,
title = {{Emergence of Nonlocal Hydrodynamics in Many-Body Radiative Heat Transport}},
author = {Mauricio Gomez Viloria and Florian Herz and Riccardo Messina and Philippe Ben-Abdallah},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.16488},
eprint = {2610.16488},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.16488},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Emergence of Nonlocal Hydrodynamics in Many-Body Radiative Heat Transport
AU - Mauricio Gomez Viloria
AU - Florian Herz
AU - Riccardo Messina
AU - Philippe Ben-Abdallah
PY - 2026
DA - 2026/10/12
PB - arXiv
DO - 10.48550/arxiv.2610.16488
UR - https://arxiv.org/abs/2610.16488
AB - We develop a nonlocal hydrodynamic theory of radiative heat transport in many-body systems by coarse graining their microscopic electrodynamic interactions. Long-range radiative exchange naturally generates a spatially nonlocal constitutive relation in which the heat current at a given position depends on temperature gradients over an extended region, while energy conservation retains its local conservative form. Fourier transport emerges as a controlled long-wavelength limit when the interaction kernel has a finite second spatial moment. When this moment fails to converge, spatial nonlocality survives coarse graining and gives rise to non-Fourier transport. The resulting framework establishes a systematic bridge between discrete many-body fluctuational electrodynamics and a continuous description of radiative heat transport.
ER -