Correlations in Perturbed Dual-Unitary Circuits: Efficient Path-Integral Formula

Interacting many-body systems with explicitly accessible spatiotemporal correlation functions are extremely rare, especially in the absence of Bethe-ansatz or Yang-Baxter integrability. Recently, we identified a remarkable class of such systems and termed them dual-unitary quantum circuits. These ar...

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Autores principales: Pavel Kos, Bruno Bertini, Tomaž Prosen
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Publicado: American Physical Society 2021
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spelling oai:doaj.org-article:b60e2cfaf32a423096fc1efc455839132021-12-02T14:37:47ZCorrelations in Perturbed Dual-Unitary Circuits: Efficient Path-Integral Formula10.1103/PhysRevX.11.0110222160-3308https://doaj.org/article/b60e2cfaf32a423096fc1efc455839132021-02-01T00:00:00Zhttp://doi.org/10.1103/PhysRevX.11.011022http://doi.org/10.1103/PhysRevX.11.011022https://doaj.org/toc/2160-3308Interacting many-body systems with explicitly accessible spatiotemporal correlation functions are extremely rare, especially in the absence of Bethe-ansatz or Yang-Baxter integrability. Recently, we identified a remarkable class of such systems and termed them dual-unitary quantum circuits. These are brickwork-type local quantum circuits whose dynamics are unitary in both time and space. The spatiotemporal correlation functions of these systems turn out to be nontrivial only at the edge of the causal light cone and can be computed in terms of one-dimensional transfer matrices. Dual unitarity, however, requires fine-tuning, and the degree of generality of the observed dynamical features remains unclear. Here, we address this question by studying perturbed dual-unitary quantum circuits. Considering arbitrary perturbations of the local gates, we prove that for a particular class of unperturbed elementary dual-unitary gates the correlation functions are still expressed in terms of one-dimensional transfer matrices. These matrices, however, are now contracted over generic paths connecting the origin to a fixed end point inside the causal light cone. The correlation function is given as a sum over all such paths. Our statement is rigorous in the “dilute limit,” where only a small fraction of the gates is perturbed, and in the presence of random longitudinal fields, but we provide theoretical arguments and stringent numerical checks supporting its validity even in the clean case (no randomness) and when all gates are perturbed. As a by-product of our analysis, in the case of random longitudinal fields—which turns out to be equivalent to certain classical Markov chains—we find four types of non-dual-unitary (and nonintegrable) interacting many-body systems where the correlation functions are exactly solvable and given—without approximations—by the path-sum formula.Pavel KosBruno BertiniTomaž ProsenAmerican Physical SocietyarticlePhysicsQC1-999ENPhysical Review X, Vol 11, Iss 1, p 011022 (2021)
institution DOAJ
collection DOAJ
language EN
topic Physics
QC1-999
spellingShingle Physics
QC1-999
Pavel Kos
Bruno Bertini
Tomaž Prosen
Correlations in Perturbed Dual-Unitary Circuits: Efficient Path-Integral Formula
description Interacting many-body systems with explicitly accessible spatiotemporal correlation functions are extremely rare, especially in the absence of Bethe-ansatz or Yang-Baxter integrability. Recently, we identified a remarkable class of such systems and termed them dual-unitary quantum circuits. These are brickwork-type local quantum circuits whose dynamics are unitary in both time and space. The spatiotemporal correlation functions of these systems turn out to be nontrivial only at the edge of the causal light cone and can be computed in terms of one-dimensional transfer matrices. Dual unitarity, however, requires fine-tuning, and the degree of generality of the observed dynamical features remains unclear. Here, we address this question by studying perturbed dual-unitary quantum circuits. Considering arbitrary perturbations of the local gates, we prove that for a particular class of unperturbed elementary dual-unitary gates the correlation functions are still expressed in terms of one-dimensional transfer matrices. These matrices, however, are now contracted over generic paths connecting the origin to a fixed end point inside the causal light cone. The correlation function is given as a sum over all such paths. Our statement is rigorous in the “dilute limit,” where only a small fraction of the gates is perturbed, and in the presence of random longitudinal fields, but we provide theoretical arguments and stringent numerical checks supporting its validity even in the clean case (no randomness) and when all gates are perturbed. As a by-product of our analysis, in the case of random longitudinal fields—which turns out to be equivalent to certain classical Markov chains—we find four types of non-dual-unitary (and nonintegrable) interacting many-body systems where the correlation functions are exactly solvable and given—without approximations—by the path-sum formula.
format article
author Pavel Kos
Bruno Bertini
Tomaž Prosen
author_facet Pavel Kos
Bruno Bertini
Tomaž Prosen
author_sort Pavel Kos
title Correlations in Perturbed Dual-Unitary Circuits: Efficient Path-Integral Formula
title_short Correlations in Perturbed Dual-Unitary Circuits: Efficient Path-Integral Formula
title_full Correlations in Perturbed Dual-Unitary Circuits: Efficient Path-Integral Formula
title_fullStr Correlations in Perturbed Dual-Unitary Circuits: Efficient Path-Integral Formula
title_full_unstemmed Correlations in Perturbed Dual-Unitary Circuits: Efficient Path-Integral Formula
title_sort correlations in perturbed dual-unitary circuits: efficient path-integral formula
publisher American Physical Society
publishDate 2021
url https://doaj.org/article/b60e2cfaf32a423096fc1efc45583913
work_keys_str_mv AT pavelkos correlationsinperturbeddualunitarycircuitsefficientpathintegralformula
AT brunobertini correlationsinperturbeddualunitarycircuitsefficientpathintegralformula
AT tomazprosen correlationsinperturbeddualunitarycircuitsefficientpathintegralformula
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