Fate of dissipative hierarchy of timescales in the presence of unitary
dynamics
- URL: http://arxiv.org/abs/2304.09017v2
- Date: Fri, 9 Feb 2024 15:39:45 GMT
- Title: Fate of dissipative hierarchy of timescales in the presence of unitary
dynamics
- Authors: Nick D. Hartmann, Jimin L. Li, David J. Luitz
- Abstract summary: generic behavior of purely dissipative open quantum many-body systems with local dissipation processes can be investigated using random matrix theory.
Here, we analyze how this spectrum evolves when unitary dynamics is present, both for the case of strongly and weakly dissipative dynamics.
For the physically most relevant case of (dissipative) two-body interactions, we find that the correction in the first order of the perturbation vanishes.
For weak dissipation, the spectrum flows into clusters with well-separated eigenmodes, which we identify to be the local symmetries of the Hamiltonian.
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- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: The generic behavior of purely dissipative open quantum many-body systems
with local dissipation processes can be investigated using random matrix
theory, revealing a hierarchy of decay timescales of observables organized by
their complexity as shown in [Wang et al., Phys. Rev. Lett. 124, 100604
(2020)]. This hierarchy is reflected in distinct eigenvalue clusters of the
Lindbladian. Here, we analyze how this spectrum evolves when unitary dynamics
is present, both for the case of strongly and weakly dissipative dynamics. In
the strongly dissipative case, the unitary dynamics can be treated
perturbatively and it turns out that the locality of the Hamiltonian determines
how susceptible the spectrum is to such a perturbation. For the physically most
relevant case of (dissipative) two-body interactions, we find that the
correction in the first order of the perturbation vanishes, leading to the
relative robustness of the spectral features. For weak dissipation, the
spectrum flows into clusters with well-separated eigenmodes, which we identify
to be the local symmetries of the Hamiltonian.
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