2019
DOI: 10.1103/physrevlett.123.230606
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Bounds on Chaos from the Eigenstate Thermalization Hypothesis

Abstract: We show that known bounds on the growth rates of operator complexity and the out-of-timeorder four-point correlator in chaotic many-body quantum systems follow directly from the general structure of operator matrix elements in systems that obey the eigenstate thermalization hypothesis. This ties together two key paradigms of thermal behavior in isolated many-body quantum systems.

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Cited by 130 publications
(98 citation statements)
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“…It is interesting to note that, as λ L is defined via a four-point correlation function (the OTOC), while α depends on a two-point correlation function (C(t)), the bound (37) can be interpreted as a relation between correlation functions of distinct nature. Such a relation is, to our knowledge, rather unusual (see [50] for a recent result). However, this point of view is not how we derived (37); an alternative proof working directly with the correlation functions would be illuminating.…”
Section: Growth Rate As a Bound On Chaosmentioning
confidence: 77%
“…It is interesting to note that, as λ L is defined via a four-point correlation function (the OTOC), while α depends on a two-point correlation function (C(t)), the bound (37) can be interpreted as a relation between correlation functions of distinct nature. Such a relation is, to our knowledge, rather unusual (see [50] for a recent result). However, this point of view is not how we derived (37); an alternative proof working directly with the correlation functions would be illuminating.…”
Section: Growth Rate As a Bound On Chaosmentioning
confidence: 77%
“…Both the bounds on this rate and the Lyapunov exponent were shown to follow from the eigenstate thermalization hypothesis in Ref. [17]. (13) The circuit complexity was suggested to be related to the logarithm of the Loschmidt echo in Ref.…”
Section: A Spectral Form Factormentioning
confidence: 99%
“…Definida c o mo [A(0), B(t)], essa quantidade mede a influência d e u m a perturbação causada pelo operador A, sobre uma medida posterior do operador B, e sua dependência temporal é sens´ıvel à dinâmica clássica [14]. Aliás, os dois problemas parecem estar relacionados [15].…”
Section: Sistemas Caóticosunclassified