Entanglement distribution in fermion model with long-range interaction
arXiv:2203.10277 · doi:10.1103/PhysRevB.107.235129
Abstract
How two-party entanglement (TPE) is distributed in the many-body systems? This is a fundamental issue because the total TPE between one party with all the other parties, , is upper bounded by the Coffman, Kundu and Wootters (CKW) monogamy inequality, from which can be proved by the geometric inequality. Here we explore the total entanglement and the associated total tangle in a -wave free fermion model with long-range interaction, showing that and may become vanishing small with the increasing of long-range interaction. However, we always find , where is the truncation length of entanglement, beyond which the TPE is quickly vanished, hence . This relation is a direct consequence of the exponential decay of the TPE induced by the long-range interaction. These results unify the results in the Lipkin-Meshkov-Glick (LMG) model and Dicke model and generalize the Koashi, Buzek and Imono bound to the quantum many-body models, with much broader applicability.
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