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Disentangling ( 2 + 1 ) D topological states of matter with entanglement negativity
We use the entanglement negativity, a bipartite measure of entanglement in mixed quantum states, to study how multipartite entanglement constrains the real-space structure of the ground-state wave functions of ( 2 + 1 ) -dimensional topological phases. We focus on the (Abelian) Laughlin and (non-Abe...
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Published in: | Physical review. B 2021-09, Vol.104 (11), p.1, Article 115155 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We use the entanglement negativity, a bipartite measure of entanglement in mixed quantum states, to study how multipartite entanglement constrains the real-space structure of the ground-state wave functions of ( 2 + 1 ) -dimensional topological phases. We focus on the (Abelian) Laughlin and (non-Abelian) Moore-Read states at filling fraction ν = 1 / m . We show that a combination of entanglement negativities, calculated with respect to specific cylinder and torus geometries, determines a necessary condition for when a topological state can be disentangled, i.e., factorized into a tensor product of states defined on cylinder subregions. This condition, which requires the ground state to lie in a definite topological sector, is sufficient for the Laughlin state. On the other hand, we find that a general Moore-Read ground state cannot be disentangled even when the disentangling condition holds. |
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ISSN: | 2469-9950 2469-9969 |
DOI: | 10.1103/PhysRevB.104.115155 |