In the Z3 chiral clock model, DQPTs emerge only for special angles in the chiral phase, with an analytical expression derived for the zeros of the dynamical partition function.
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In a mean-field driven lattice gas with obstacle, a nonequilibrium transition creates local invariants that shield the obstacle complex from external drive fluctuations and localize noise-induced fluctuations near the phase domain wall.
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Emergent dynamical quantum phase transition in a $Z_3$ symmetric chiral clock model
In the Z3 chiral clock model, DQPTs emerge only for special angles in the chiral phase, with an analytical expression derived for the zeros of the dynamical partition function.
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Nonequilibrium protection effect and spatial localization of noise-induced fluctuations: Quasi-one-dimensional driven lattice gas with partially penetrable obstacle
In a mean-field driven lattice gas with obstacle, a nonequilibrium transition creates local invariants that shield the obstacle complex from external drive fluctuations and localize noise-induced fluctuations near the phase domain wall.