A (1+1)D SU(2) lattice gauge theory with dynamical matter exhibits ergodic, fragmented, and disorder-free many-body localized phases under non-Abelian gauge constraints, with the localized regime preserving spatial inhomogeneities via sector superpositions.
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For algebraic quenches in the 1D TFIM, the longitudinal kink-kink correlator depends only on the KZ length for superlinear cases and otherwise needs a dephasing length, decaying as a compressed exponential with exponent varying continuously with the quench exponent.
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Kink-kink correlations in nonlinear quenches across a quantum critical point
For algebraic quenches in the 1D TFIM, the longitudinal kink-kink correlator depends only on the KZ length for superlinear cases and otherwise needs a dephasing length, decaying as a compressed exponential with exponent varying continuously with the quench exponent.