Disordered orbital Hatsugai-Kohmoto model shows a transition from Poisson to GOE level statistics as interaction disorder increases, while OTOC plateau values fail to uniformly distinguish chaos across models.
Randomness and Chaos in Qubit Models
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abstract
We introduce randomness into a class of integrable models and study the spectral form factor as a diagnostic to distinguish between randomness and chaos. Spectral form factors exhibit a characteristic dip-ramp-plateau behavior in the $N>2$ SYK$_2$ model at high temperatures that is absent in the $N=2$ SYK$_2$ model. Our results suggest that this dip-ramp-plateau behavior implies the existence of random eigenvectors in a quantum many-body system. To further support this observation, we examine the Gaussian random transverse Ising model and obtain consistent results without suffering from small $N$ issues. Finally, we demonstrate numerically that expectation values of observables computed in a random quantum state at late times are equivalent to the expectation values computed in the thermal ensemble in a Gaussian random one-qubit model.
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Chaotic-Integrable Transition for Disordered Orbital Hatsugai-Kohmoto Model
Disordered orbital Hatsugai-Kohmoto model shows a transition from Poisson to GOE level statistics as interaction disorder increases, while OTOC plateau values fail to uniformly distinguish chaos across models.