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Fast mixing of weakly interacting fermionic systems at any temperature
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We study the mixing time of a recently proposed efficiently implementable Lindbladian designed to prepare the Gibbs states in the setting of weakly interacting fermionic systems. We show that at any temperature, the Lindbladian spectral gap for even parity observables is lower bounded by a constant that is independent of the system size, when the interaction strength (e.g., the on-site interaction strength for the Fermi-Hubbard model) is below a constant threshold, which is also independent of the system size. This leads to a mixing time estimate that is at most linear in the system size, thus showing that the corresponding Gibbs states can be prepared efficiently on quantum computers.
Forward citations
Cited by 2 Pith papers
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A cluster-expansion FPTAS for the partition function and an approximate sampler for weakly-interacting quantum spin systems at arbitrary temperature are claimed, but a key bound in the proof fails.
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