Saved in:
Bibliographic Details
Main Authors: Solanki, Parvinder, Minganti, Fabrizio
Format: Preprint
Published: 2024
Subjects:
Online Access:https://arxiv.org/abs/2411.07297
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866908605059432448
author Solanki, Parvinder
Minganti, Fabrizio
author_facet Solanki, Parvinder
Minganti, Fabrizio
contents While a generic open quantum system decays to its steady state, continuous time crystals (CTCs) develop spontaneous oscillation and never converge to a stationary state. Just as crystals develop correlations in space, CTCs do so in time. Here, we introduce a Continuous Quasi Time Crystals (CQTC). Despite being characterized by the presence of non-decaying oscillations, this phase does not retain its long-range order, making it the time analogous of quasi-crystal structures. We investigate the emergence of this phase in a system made of two coupled collective spin sub-systems, each developing a CTC phase upon the action of a strong enough drive. The addition of a coupling enables the emergence of different synchronized phases, where both sub-systems oscillate at the same frequency. In the transition between different CTC orders, the system develops chaotic dynamics with aperiodic oscillations. These chaotic features differ from those of closed quantum systems, as the dynamics is not characterized by a unitary evolution. At the same time, the presence of non-decaying oscillations makes this phenomenon distinct from other form of chaos in open quantum system, where the system decays instead. We investigate the connection between chaos and this quasi-crystalline phase using mean-field techniques, and we confirm these results including quantum fluctuations at the lowest order.
format Preprint
id arxiv_https___arxiv_org_abs_2411_07297
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Chaos in Time: A Dissipative Continuous Quasi Time Crystals
Solanki, Parvinder
Minganti, Fabrizio
Quantum Physics
Statistical Mechanics
While a generic open quantum system decays to its steady state, continuous time crystals (CTCs) develop spontaneous oscillation and never converge to a stationary state. Just as crystals develop correlations in space, CTCs do so in time. Here, we introduce a Continuous Quasi Time Crystals (CQTC). Despite being characterized by the presence of non-decaying oscillations, this phase does not retain its long-range order, making it the time analogous of quasi-crystal structures. We investigate the emergence of this phase in a system made of two coupled collective spin sub-systems, each developing a CTC phase upon the action of a strong enough drive. The addition of a coupling enables the emergence of different synchronized phases, where both sub-systems oscillate at the same frequency. In the transition between different CTC orders, the system develops chaotic dynamics with aperiodic oscillations. These chaotic features differ from those of closed quantum systems, as the dynamics is not characterized by a unitary evolution. At the same time, the presence of non-decaying oscillations makes this phenomenon distinct from other form of chaos in open quantum system, where the system decays instead. We investigate the connection between chaos and this quasi-crystalline phase using mean-field techniques, and we confirm these results including quantum fluctuations at the lowest order.
title Chaos in Time: A Dissipative Continuous Quasi Time Crystals
topic Quantum Physics
Statistical Mechanics
url https://arxiv.org/abs/2411.07297