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Thermalization in the mixed-field Ising model: An occupation-number perspective
Isaías Vallejo-Fabila1, Fausto Borgonovi2,3, Felix M Izrailev4,5
1University of Connecticut, Department of Physics, Storrs, Connecticut 06269, USA.
We studied thermalization in quantum and classical spin models using occupation numbers. Classical ergodicity deviations decay algebraically, providing bounds for quantum thermalization.
Area of Science:
- Statistical Mechanics
- Quantum Physics
- Condensed Matter Theory
Background:
- Occupation number is crucial for understanding thermalization and statistical distributions (Fermi-Dirac, Bose-Einstein, Boltzmann).
- In spin systems, it quantifies magnetization sublevel populations.
- Probing thermalization in isolated quantum spin models is challenging due to Hilbert space size.
Purpose of the Study:
- To investigate the onset of thermalization in a quantum spin-1 Ising model and its classical counterpart.
- To establish a quantitative criterion for ergodicity in interacting spin systems.
- To determine bounds for the approach to thermal equilibrium in quantum models.
Main Methods:
- Analyzed the occupation number dynamics in a 1D quantum spin-1 Ising model with transverse and longitudinal fields.
- Utilized the classical counterpart to overcome finite-size limitations in quantum simulations.
- Tracked individual spin dynamics on Bloch spheres and applied random matrix theory.
Main Results:
- Thermalization in the quantum model was assessed by the convergence of occupation number averages to microcanonical predictions.
- Classical ergodicity deviations were found to decay algebraically with system size (power-law scaling).
- This scaling provided a quantitative bound for the approach to thermal equilibrium in the quantum system.
Conclusions:
- The study establishes a link between classical ergodicity and quantum thermalization.
- Algebraic decay of classical ergodicity provides a practical method to bound quantum thermalization.
- The findings offer insights into the dynamics and equilibrium properties of isolated spin systems.
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