Long coherence times for edge spins

We show that in certain one-dimensional spin chains with open boundary conditions, the edge spins retain memory of their initial state for very long times, even at infinite temperature. The long coherence times do not require disorder, only an ordered phase. In the integrable Ising and XYZ chains, t...

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Bibliografski detalji
Glavni autori: Kemp, J, Yao, N, Laumann, C, Fendley, P
Format: Journal article
Izdano: Institute of Physics 2017
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author Kemp, J
Yao, N
Laumann, C
Fendley, P
author_facet Kemp, J
Yao, N
Laumann, C
Fendley, P
author_sort Kemp, J
collection OXFORD
description We show that in certain one-dimensional spin chains with open boundary conditions, the edge spins retain memory of their initial state for very long times, even at infinite temperature. The long coherence times do not require disorder, only an ordered phase. In the integrable Ising and XYZ chains, the presence of a strong zero mode means the coherence time is infinite. When Ising is perturbed by interactions breaking the integrability, the coherence time remains exponentially long in the perturbing couplings. We show that this is a consequence of an edge “almost” strong zero mode that almost commutes with the Hamiltonian. We compute this operator explicitly, allowing us to estimate accurately the plateau value of edge spin autocorrelator.
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spelling oxford-uuid:a1557933-5263-4349-8a12-16a00f15a5212022-03-27T02:12:23ZLong coherence times for edge spinsJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:a1557933-5263-4349-8a12-16a00f15a521Symplectic Elements at OxfordInstitute of Physics2017Kemp, JYao, NLaumann, CFendley, PWe show that in certain one-dimensional spin chains with open boundary conditions, the edge spins retain memory of their initial state for very long times, even at infinite temperature. The long coherence times do not require disorder, only an ordered phase. In the integrable Ising and XYZ chains, the presence of a strong zero mode means the coherence time is infinite. When Ising is perturbed by interactions breaking the integrability, the coherence time remains exponentially long in the perturbing couplings. We show that this is a consequence of an edge “almost” strong zero mode that almost commutes with the Hamiltonian. We compute this operator explicitly, allowing us to estimate accurately the plateau value of edge spin autocorrelator.
spellingShingle Kemp, J
Yao, N
Laumann, C
Fendley, P
Long coherence times for edge spins
title Long coherence times for edge spins
title_full Long coherence times for edge spins
title_fullStr Long coherence times for edge spins
title_full_unstemmed Long coherence times for edge spins
title_short Long coherence times for edge spins
title_sort long coherence times for edge spins
work_keys_str_mv AT kempj longcoherencetimesforedgespins
AT yaon longcoherencetimesforedgespins
AT laumannc longcoherencetimesforedgespins
AT fendleyp longcoherencetimesforedgespins