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arXiv: 2102.13452
handle: 10261/278423
The dynamics of open quantum systems can be described by a Liouvillian, which in the Markovian approximation fulfills the Lindblad master equation. We present a family of integrable many-body Liouvillians based on Richardson-Gaudin models with a complex structure of the jump operators. Making use of this new region of integrability, we study the transition to chaos in terms of a two-parameter Liouvillian. The transition is characterized by the spectral statistics of the complex eigenvalues of the Liouvillian operators using the nearest neighbor spacing distribution and by the ratios between eigenvalue distances.
Quantum Physics, Nonlinear Sciences - Exactly Solvable and Integrable Systems, Statistical Mechanics (cond-mat.stat-mech), Strongly Correlated Electrons (cond-mat.str-el), Physics, QC1-999, FOS: Physical sciences, Nonlinear Sciences - Chaotic Dynamics, Condensed Matter - Strongly Correlated Electrons, Chaotic Dynamics (nlin.CD), Exactly Solvable and Integrable Systems (nlin.SI), Quantum Physics (quant-ph), Condensed Matter - Statistical Mechanics
Quantum Physics, Nonlinear Sciences - Exactly Solvable and Integrable Systems, Statistical Mechanics (cond-mat.stat-mech), Strongly Correlated Electrons (cond-mat.str-el), Physics, QC1-999, FOS: Physical sciences, Nonlinear Sciences - Chaotic Dynamics, Condensed Matter - Strongly Correlated Electrons, Chaotic Dynamics (nlin.CD), Exactly Solvable and Integrable Systems (nlin.SI), Quantum Physics (quant-ph), Condensed Matter - Statistical Mechanics
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