Energy distribution and local fluctuations in strongly coupled open quantum systems: The extended resonant level model
Maicol A. Ochoa, Anton Bruch, Abraham Nitzan

TL;DR
This paper investigates the limitations of dividing the Hamiltonian in strongly coupled open quantum systems to describe energy fluctuations and thermodynamics, showing that such splitting generally fails beyond equilibrium and wide-band approximations.
Contribution
The study demonstrates that symmetric splitting of the interaction Hamiltonian cannot accurately describe energy fluctuations or thermodynamics in strongly coupled quantum systems beyond equilibrium.
Findings
Splitting fails to capture energy fluctuations at equilibrium.
No subsystem division can fully describe energy distribution.
Splitting approach is invalid without wide-band approximation.
Abstract
We study the energy distribution in the extended resonant level model at equilibrium. Previous investigations [Phys. Rev. B {\bf 89}, 161306 (2014), Phys. Rev. B {\bf 93}, 115318 (2016)] have found, for a resonant electronic level interacting with a thermal free electron wide-band bath, that the expectation value for the energy of the interacting subsystem can be correctly calculated by considering a symmetric splitting of the interaction Hamiltonian between the subsystem and the bath. However, the general implications of this approach were questioned [Phys. Rev. B {\bf 92}, 235440 (2015)]. Here we show that already at equilibrium, such splitting fails to describe the energy fluctuations, as measured here by the second and third central moments (namely width and skewness) of the energy distribution. Furthermore, we find that when the wide-band approximation does not hold, no splitting…
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