Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/8075
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dc.contributor.authorSREERAM, P. G.en_US
dc.contributor.authorModak, Ranjanen_US
dc.contributor.authorAravinda, S.en_US
dc.date.accessioned2023-07-21T10:38:05Z
dc.date.available2023-07-21T10:38:05Z
dc.date.issued2023-06en_US
dc.identifier.citationPhysical Review E, 107(06), 064204.en_US
dc.identifier.issn2470-0045en_US
dc.identifier.issn2470-0053en_US
dc.identifier.urihttps://doi.org/10.1103/PhysRevE.107.064204en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/8075
dc.description.abstractWe study observation entropy (OE) for the quantum kicked top model, whose classical counterpart possesses different phases: regular, mixed, or chaotic, depending on the strength of the kicking parameter. We show that OE grows logarithmically with coarse-graining length beyond a critical value in the regular phase, while OE growth is much faster in the chaotic regime. In the dynamics, we demonstrate that the short-time growth rate of OE acts as a measure of the chaoticity in the system, and we compare our results with out-of-time-ordered correlators (OTOC). Moreover, we show that in the deep quantum regime, the results obtained from OE are much more robust compared to OTOC results. Finally, we also investigate the long-time behavior of OE to distinguish between saddle-point scrambling and true chaos, where the former shows large persistent fluctuations compared to the latter.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectThermalizationen_US
dc.subjectHundredsen_US
dc.subjectDynamicsen_US
dc.subject2023-JUL-WEEK2en_US
dc.subjectTOC-JUL-2023en_US
dc.subject2023en_US
dc.titleWitnessing quantum chaos using observational entropyen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Een_US
dc.publication.originofpublisherForeignen_US
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