For strong disorder the root-averaged density of states of the Anderson model on the Bethe lattice is absolutely continuous with real-analytic density possessing a finite-order strong-disorder expansion whose leading coefficient is the single-site density and whose odd coefficients all vanish.
Statistical theory of superlattices
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Quantum jump correlations and waiting-time distributions in long-range dissipative spins display clear signatures of the paramagnetic-to-ferromagnetic transition when analyzed with tilted Lindbladian, cluster mean-field, and cumulant expansion methods.
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Strong-disorder expansion of the root-averaged density of states for the Anderson model on the Bethe lattice
For strong disorder the root-averaged density of states of the Anderson model on the Bethe lattice is absolutely continuous with real-analytic density possessing a finite-order strong-disorder expansion whose leading coefficient is the single-site density and whose odd coefficients all vanish.
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Quantum jump correlations in long-range dissipative spin systems via cluster and cumulant expansions
Quantum jump correlations and waiting-time distributions in long-range dissipative spins display clear signatures of the paramagnetic-to-ferromagnetic transition when analyzed with tilted Lindbladian, cluster mean-field, and cumulant expansion methods.