A bosonic perspective on the classical mapping of fermionic quantum dynamics
Jing Sun, Sudip Sasmal, Oriol Vendrell

TL;DR
This paper explores the classical mapping of fermionic quantum dynamics using the Meyer-Miller Hamiltonian, comparing it with other mappings, and finds that the MM mapping can accurately reproduce one-body density dynamics even in interacting systems.
Contribution
It demonstrates that the Meyer-Miller classical mapping is exact for non-interacting fermions and compares its performance with other fermionic mappings, revealing its effectiveness in complex models.
Findings
MM mapping is exact for non-interacting fermions.
Including fermionic anti-symmetry via Jordan-Wigner does not improve mapping accuracy.
MM and LMM mappings can capture interference effects in energy transfer models.
Abstract
We consider the application of the original Meyer-Miller (MM) Hamiltonian to mapping fermionic quantum dynamics to classical equations of motion. Non-interacting fermionic and bosonic systems share the same one-body density dynamics when evolving from the same initial many-body state. The MM classical mapping is exact for non-interacting bosons, and therefore it yields the exact time-dependent one-body density for non-interacting fermions as well. Starting from this observation, the MM mapping is compared to different mappings specific for fermionic systems, namely the spin mapping (SM) with and without including a Jordan-Wigner transformation, and the Li-Miller mapping (LMM). For non-interacting systems, the inclusion of fermionic anti-symmetry through the Jordan-Wigner transform does not lead to any improvement in the performance of the mappings and instead it worsens the classical…
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