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Since Si(ω) is sharply peaked for a specific disorder realization in the localized regime, we choose the median frequency as the oscillating frequency of spini

For both figures, we consider a single disorder realization atW= 4, L= 10 product state|ψ 0⟩ Si(ω) = 2πs z i X mn cmc∗ n(σz i )mnδ(ω+E m −E n) (12) whereσ z i (0)|ψ0⟩=s z i |ψ0⟩, c

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Coherently synchronized oscillations in many-body localization

cond-mat.dis-nn · 2025-12-12 · unverdicted · novelty 6.0

Coherently synchronized oscillations appear in mirror-symmetric MBL systems and undergo a synchronization transition that maps to a paramagnetic-ferromagnetic Ising transition in an effective model built from local integrals of motion.

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  • Coherently synchronized oscillations in many-body localization cond-mat.dis-nn · 2025-12-12 · unverdicted · none · ref 1

    Coherently synchronized oscillations appear in mirror-symmetric MBL systems and undergo a synchronization transition that maps to a paramagnetic-ferromagnetic Ising transition in an effective model built from local integrals of motion.