In the non-Hermitian transverse-field Ising model, dissipation causes defect density to exhibit Kibble-Zurek, anti-Kibble-Zurek, or super-Kibble-Zurek scaling due to excitations across broad momentum sectors rather than only near gap closing.
Separation of the Kibble-Zurek Mechanism from Quantum Criticality
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abstract
When a system is swept through a quantum critical point (QCP), the Kibble-Zurek mechanism predicts that the average number of topological defects follows a universal power-law scaling with the ramp time scale. This scaling behavior is determined by the equilibrium critical exponents of the underlying phase transition. We show that the correspondence between Kibble-Zurek scaling and quantum criticality does not hold generally. In particular, the defect density can exhibit a suppression faster than the Kibble-Zurek prediction even when the quench crosses a critical point, while conventional Kibble-Zurek scaling may persist for quenches through a non-critical point. Our results, based on models representative of a broad class of quasi-one-dimensional Fermi systems, identify the dynamical conditions under which universal defect scaling emerges and clarify the relation between defect generation and equilibrium criticality.
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quant-ph 1years
2026 1verdicts
UNVERDICTED 1representative citing papers
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Dissipation-Induced Deviations from Kibble-Zurek Scaling in Non-Hermitian Quantum Annealing
In the non-Hermitian transverse-field Ising model, dissipation causes defect density to exhibit Kibble-Zurek, anti-Kibble-Zurek, or super-Kibble-Zurek scaling due to excitations across broad momentum sectors rather than only near gap closing.