2016
DOI: 10.48550/arxiv.1604.02743
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Dynamical complexity in the quantum to classical transition

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Cited by 5 publications
(13 citation statements)
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“…There were recent reports of emergence of chaos in the quantum regime in absence of classical chaos. 77,78 In these works, the quantum versus classical "weights" of the system is controlled by the effective Planck constant, where the classical limit is reached when the constant approaches zero. In our system, the parameter g 0 plays the same role.…”
Section: Remark 1: Transient Chaos In Quantum Systems -What Does It M...mentioning
confidence: 99%
“…There were recent reports of emergence of chaos in the quantum regime in absence of classical chaos. 77,78 In these works, the quantum versus classical "weights" of the system is controlled by the effective Planck constant, where the classical limit is reached when the constant approaches zero. In our system, the parameter g 0 plays the same role.…”
Section: Remark 1: Transient Chaos In Quantum Systems -What Does It M...mentioning
confidence: 99%
“…In particular, the study of the effects of the coupling details on the chaotic behaviour [11] and of puzzling results in optomechanics [12] have provided with very interesting advances. In this context, quantum chaotic attractors with apparently no classical counterpart have been found in the open dissipative quantum Duffing system [13]. On the other hand, despite known discrepancies [16,25] for some limited cases and surviving quantum effects, effective classical maps with Gaussian noise have been proposed as a direct replacement to obtain the main features of quantum dissipative systems.…”
Section: Discussionmentioning
confidence: 99%
“…Finally, it was recently claimed that quantum chaotic attractors (i.e. complex quantum equilibrium states typically associated to classical chaotic attractors) with no classical * carlo@tandar.cnea.gov.ar counterpart exist in the open dissipative quantum Duffing system [13].…”
Section: Introductionmentioning
confidence: 99%
“…In the former case, the evolution approaches that of the probability density in phase space for the equivalent classical system as the action is increased [4,7,15]. Continuous observation turns this probability density into individual trajectories that follow the nonlinear classical motion with the requisite Lyapunov exponents [12,15,17,18].…”
mentioning
confidence: 98%
“…There has been a great deal of interest in purely quantum systems, displaying unitary evolution, and non-unitary open quantum systems. This paper is concerned with open quantum systems whose classical counterparts are chaotic and make a transition to chaotic behavior as their size (more precisely their action) is increased so as to be large compared to [2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19]. This transition is enabled by their interaction with the environment or when they are subjected to continuous observation.…”
mentioning
confidence: 99%