Transport Determines Spectral Distance in Mesoscopic Thermodynamics
Abstract
We derive a distance between thermodynamic states from a positive Hermitian transport tensor within a mesoscopic canonical model. An exact first-order factorization of the evolution generator gives a commutator norm and the metric G=2g, where g denotes the symmetric transport tensor. Gradients of the antisymmetric tensor can change the evolution, but they leave this distance unchanged. The construction allows coordinate-dependent coefficients. For constant Onsager coefficients, a Clifford representation gives the same metric. In a two-channel thermoelectric system, the ratio of normalized principal distances is √(1+ZT)+√(ZT). Transport coupling thus fixes the anisotropy of this metric. The construction requires neither an independent metric nor a physical spin variable.
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BibTeX
@misc{sonnino2026transport,
title = {{Transport Determines Spectral Distance in Mesoscopic Thermodynamics}},
author = {Giorgio SONNINO},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.16752},
eprint = {2610.16752},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.16752},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Transport Determines Spectral Distance in Mesoscopic Thermodynamics
AU - Giorgio SONNINO
PY - 2026
DA - 2026/10/18
PB - arXiv
DO - 10.48550/arxiv.2610.16752
UR - https://arxiv.org/abs/2610.16752
AB - We derive a distance between thermodynamic states from a positive Hermitian transport tensor within a mesoscopic canonical model. An exact first-order factorization of the evolution generator gives a commutator norm and the metric G=2g, where g denotes the symmetric transport tensor. Gradients of the antisymmetric tensor can change the evolution, but they leave this distance unchanged. The construction allows coordinate-dependent coefficients. For constant Onsager coefficients, a Clifford representation gives the same metric. In a two-channel thermoelectric system, the ratio of normalized principal distances is √(1+ZT)+√(ZT). Transport coupling thus fixes the anisotropy of this metric. The construction requires neither an independent metric nor a physical spin variable.
ER -