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This paper refutes a recent conjecture regarding ground-state overlap dominance in quantum quenches, establishing that same-phase transitions can still be dominated by excited states in specific free-fermion systems like Kitaev chains. By deriving exact geometric conditions for momentum sectors, the work clarifies the mechanisms behind dynamical quantum phase transitions without requiring equilibrium phase boundary crossings. These findings are critical for understanding non-equilibrium dynamics in quantum many-body systems and refining theoretical models of quantum simulation protocols.
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Exact criteria for ground-state overlap dominance and dynamical quantum phase transitions

arXiv2 min read

arXiv:2604.11420v3 Announce Type: replace-cross Abstract: It was recently conjectured and verified for the transverse-field Ising model [Phys. Rev. B 113, 165102 (2026)] that, after a sudden quench within the same equilibrium phase, the initial ground state has its largest overlap with the final ground state. We show that this phase-based criterion is generally false, even in translationally invariant free-fermion systems. For Hamiltonians that factorize into independent $2\times 2$ momentum sectors, we derive the exact necessary-and-sufficient condition for ground-state overlap dominance: the initial and final sector Bloch vectors must have positive dot product for every momentum. This result proves the conjecture in classes where same-phase quenches enforce this geometric condition, but gives explicit same-phase counterexamples in Kitaev chains, where excited final eigenstates can dominate the overlap distribution. We further show that the same obstruction controls real-time Fisher-zero crossings, allowing dynamical quantum phase transitions without crossing an equilibrium phase boundary.

Abstract:It was recently conjectured and verified for the transverse-field Ising model [Phys. Rev. B 113, 165102 (2026)] that, after a sudden quench within the same equilibrium phase, the initial ground state has its largest overlap with the final ground state. We show that this phase-based criterion is generally false, even in translationally invariant free-fermion systems. For Hamiltonians that factorize into independent $2\times 2$ momentum sectors, we derive the exact necessary-and-sufficient condition for ground-state overlap dominance: the initial and final sector Bloch vectors must have positive dot product for every momentum. This result proves the conjecture in classes where same-phase quenches enforce this geometric condition, but gives explicit same-phase counterexamples in Kitaev chains, where excited final eigenstates can dominate the overlap distribution. We further show that the same obstruction controls real-time Fisher-zero crossings, allowing dynamical quantum phase transitions without crossing an equilibrium phase boundary.

Statistical Mechanics (cond-mat.stat-mech); Quantum Physics (quant-ph)

arXiv:2604.11420 [cond-mat.stat-mech]

(or arXiv:2604.11420v3 [cond-mat.stat-mech] for this version)

https://doi.org/10.48550/arXiv.2604.11420 Focus to learn more arXiv-issued DOI via DataCite

Phys. Rev. E 114, L042103 (2026)

https://doi.org/10.1103/gxlb-k4cp Focus to learn more DOI(s) linking to related resources

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Full text under the publisher's open licence · 254 words

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