Tuning a chaos parameter drives an exceptional-point transition in reset-driven Floquet channel spectra from real eigenvalues in an ergodic regime to complex pairs in a chaotic regime, distinguishing multiple dynamical phases.
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In U(1)-symmetric random circuits, initial states with lower stabilizer Rényi entropy generate nonstabilizerness faster than those with higher entropy, with the effect also depending on spatial charge structure and extending to SU(2) circuits and Hamiltonian dynamics.
Floquet strong Hilbert space fragmentation stabilizes discrete time crystals in a disorder-free kicked XXZ spin chain, with lifetime independent of frequency and exponential in system size.
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Chaos Emerge with Exceptional Points in Reset-Driven Floquet Dynamics
Tuning a chaos parameter drives an exceptional-point transition in reset-driven Floquet channel spectra from real eigenvalues in an ergodic regime to complex pairs in a chaotic regime, distinguishing multiple dynamical phases.
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Nonstabilizerness Mpemba Effects
In U(1)-symmetric random circuits, initial states with lower stabilizer Rényi entropy generate nonstabilizerness faster than those with higher entropy, with the effect also depending on spatial charge structure and extending to SU(2) circuits and Hamiltonian dynamics.
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Discrete time crystals enabled by Floquet strong Hilbert space fragmentation
Floquet strong Hilbert space fragmentation stabilizes discrete time crystals in a disorder-free kicked XXZ spin chain, with lifetime independent of frequency and exponential in system size.