Mixed-state quantum anomaly and multipartite entanglement
arXiv:2401.17357 · doi:10.1103/PhysRevX.15.011069
Abstract
Quantum entanglement measures of many-body states have been increasingly useful to characterize phases of matter. Here we explore a surprising connection between mixed state entanglement and 't Hooft anomaly. More specifically, we consider lattice systems in space dimensions with anomalous symmetry where the anomaly is characterized by an invariant in the group cohomology . We show that any mixed state that is strongly symmetric under , in the sense that , is necessarily -nonseparable, i.e. is not the mixture of tensor products of states in the Hilbert space. Furthermore, such states cannot be prepared from any -separable states using finite-depth local quantum channels, so the nonseparability is long-ranged in nature. We provide proof of these results in , and plausibility arguments in . The anomaly-nonseparability connection thus allows us to generate simple examples of mixed states with nontrivial long-ranged multipartite entanglement. In particular, in we found an example of intrinsically mixed quantum phase, in the sense that states in this phase cannot be two-way connected to any pure state through finite-depth local quantum channels. We also analyze mixed anomaly involving both strong and weak symmetries, including systems constrained by the Lieb-Schultz-Mattis type of anomaly. We find that, while strong-weak mixed anomaly in general does not constrain quantum entanglement, it does constrain long-range correlations of mixed states in nontrivial ways. Namely, such states are not symmetrically invertible and not gapped Markovian, generalizing familiar properties of anomalous pure states.
27 pages, 9 figures; New results on strong-weak mixed anomaly and other revisions
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