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Published on: June 7, 2018
Nonequilibrium Phase Transition to Temporal Oscillations in Mean-Field Spin Models
1Universite Grenoble Alpes, CNRS, LIPhy, 38000 Grenoble, France.
We developed a mean-field theory for nonequilibrium phase transitions in spin models, identifying a Hamiltonian as the key indicator of spontaneous oscillations. This theory reveals complex dynamics even without disorder.
Area of Science:
- Statistical Mechanics
- Condensed Matter Physics
- Theoretical Physics
Background:
- Understanding nonequilibrium phase transitions is crucial for complex systems.
- Spin models exhibit rich dynamical behaviors, including oscillations.
- Existing theories often struggle to capture nonequilibrium dynamics.
Purpose of the Study:
- To develop a mean-field theory for nonequilibrium phase transitions to spontaneously oscillating states in spin models.
- To identify the order parameter and characteristics of the oscillating phase.
- To provide an explicit illustration using a kinetic mean-field spin model.
Main Methods:
- Formulating a nonequilibrium generalization of Landau free energy using joint distributions.
- Defining a Hamiltonian as the order parameter for oscillations.
- Analyzing stochastic spin dynamics to determine theoretical parameters.
- Investigating overlap distributions in the oscillating phase.
Main Results:
- A novel mean-field theory for nonequilibrium phase transitions to oscillating states is proposed.
- A Hamiltonian is identified as the order parameter, signaling the onset of oscillations.
- The oscillating phase exhibits a nontrivial overlap distribution, resembling replica symmetry breaking without disorder.
Conclusions:
- The proposed mean-field theory successfully describes the transition to spontaneously oscillating states in spin models.
- The theory highlights the emergence of complex dynamics and order even in the absence of quenched disorder.
- This work provides a framework for studying nonequilibrium phenomena in magnetic systems.
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