Numerical simulations of a classical discrete anisotropic Landau-Lifshitz magnet reveal a sharp change in the infinite-temperature spin diffusion constant with perturbation strength and a crossover from non-Gaussian to Gaussian magnetization transfer statistics.
Non equilibrium quantum dynamics in ultra-cold quantum gases
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abstract
Advances in controlling and measuring systems of ultra-cold atoms provided strong motivation to theoretical investigations of quantum dynamics in closed many-body systems. Fundamental questions on quantum dynamics and statistical mechanics are now within experimental reach: How is thermalization achieved in a closed quantum system? How does quantum dynamics cross over to effective classical physics? Can such a thermal or classical fate be evaded? In these lectures, given at the Les Houches Summer School of Physics "Strongly Interacting Quantum Systems Out of Equilibrium", I introduce the students to the novel properties that make ultra-cold atomic systems a unique platform for study of non equilibrium quantum dynamics. I review a selection of recent experimental and theoretical work in which universal features and emergent phenomena in quantum dynamics are highlighted.
years
2025 2verdicts
UNVERDICTED 2representative citing papers
Periodic modulation of the trap in a unitary Fermi gas excites a dissipationless breathing mode, leading to out-of-phase energy oscillations that follow the dynamic virial theorem.
citing papers explorer
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Fate of diffusion under integrability breaking of classical integrable magnets
Numerical simulations of a classical discrete anisotropic Landau-Lifshitz magnet reveal a sharp change in the infinite-temperature spin diffusion constant with perturbation strength and a crossover from non-Gaussian to Gaussian magnetization transfer statistics.
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Energy Dynamics of a Nonequilibrium Unitary Fermi Gas
Periodic modulation of the trap in a unitary Fermi gas excites a dissipationless breathing mode, leading to out-of-phase energy oscillations that follow the dynamic virial theorem.