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This study provides a rigorous theoretical analysis of dynamical quantum phase transitions within the extended Agassi model, utilizing exact diagonalization to map non-equilibrium dynamics via Loschmidt echo scaling. The findings reveal distinct critical behaviors across different pairing channels, demonstrating that dynamical singularities do not strictly follow equilibrium transition orders and identifying specific local scaling exponents for each regime.
Nonequilibrium Dynamical Quantum Phase Transitions in the Extended Agassi Model
arXiv:2610.23096v1 Announce Type: new Abstract: We investigate dynamical quantum phase transitions (DQPTs) in the extended Agassi model following sudden quenches of same level pairing ($\Sigma$), monopole-monopole ($\chi$) and cross level pairing ($\Lambda$) strengths. Using exact diagonalization, we characterize the non-equilibrium dynamics through the Loschmidt echo and intensive return-rate function. Quenches across equilibrium phase boundaries produce cusp-like structures in the return rate that shows non-analyticities with increasing system size. Equilibrium finite size to large scaling identifies the $\chi$-driven transition as a second order phase transition similar to mean-field, Dicke, and Lipkin-Meshkov-Glick (LMG) models critical behaviour with the exponent of the order parameter $\beta \simeq 1/2$, while the $\Sigma$- and $\Lambda$-driven transitions are first order. We further characterize the associated dynamical singularities through a local scaling exponent $\alpha$, with $\alpha_\chi \simeq 2/3$, $\alpha_\Lambda \simeq 1/3$, and $\alpha_\Sigma \simeq 3/2$ of all three parameters. The distinct scaling behaviours across the parameter channels show that dynamical criticality is not determined solely by the equilibrium order of the transition, revealing multiple dynamical scaling regimes. These non-analyticities are associated with the Fisher zeros of the Loschmidt amplitude, which cross the real time axis at critical times and the time derivatives of the return-rate function to characterize the order of DQPTs within the extended Agassi model.
Abstract:We investigate dynamical quantum phase transitions (DQPTs) in the extended Agassi model following sudden quenches of same level pairing ($\Sigma$), monopole-monopole ($\chi$) and cross level pairing ($\Lambda$) strengths. Using exact diagonalization, we characterize the non-equilibrium dynamics through the Loschmidt echo and intensive return-rate function. Quenches across equilibrium phase boundaries produce cusp-like structures in the return rate that shows non-analyticities with increasing system size. Equilibrium finite size to large scaling identifies the $\chi$-driven transition as a second order phase transition similar to mean-field, Dicke, and Lipkin-Meshkov-Glick (LMG) models critical behaviour with the exponent of the order parameter $\beta \simeq 1/2$, while the $\Sigma$- and $\Lambda$-driven transitions are first order. We further characterize the associated dynamical singularities through a local scaling exponent $\alpha$, with $\alpha_\chi \simeq 2/3$, $\alpha_\Lambda \simeq 1/3$, and $\alpha_\Sigma \simeq 3/2$ of all three parameters. The distinct scaling behaviours across the parameter channels show that dynamical criticality is not determined solely by the equilibrium order of the transition, revealing multiple dynamical scaling regimes. These non-analyticities are associated with the Fisher zeros of the Loschmidt amplitude, which cross the real time axis at critical times and the time derivatives of the return-rate function to characterize the order of DQPTs within the extended Agassi model.
21 pages , 26 figures, to be submitted to journal soon. Comments will be appreciated
arXiv:2610.23096 [quant-ph]
(or arXiv:2610.23096v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2610.23096 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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Full text under the publisher's open licence · 310 words
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