Extended Order Parameter and Conjugate Field for the Dynamic Phase Transition in a Ginzburg-Landau Mean-Field Model in an Oscillating Field
arXiv:1401.6465 · doi:10.1103/PhysRevE.89.022114
Abstract
We present numerical evidence for an extended order parameter and conjugate field for the dynamic phase transition in a Ginzburg-Landau mean-field model driven by an oscillating field. The order parameter, previously taken to be the time-averaged magnetization, comprises the deviations of the Fourier components of the magnetization from their values at the critical period. The conjugate field, previously taken to be the time-averaged magnetic field, comprises the even Fourier components of the field. The scaling exponents beta and delta associated with the extended order parameter and conjugate field are shown numerically to be consistent with their values in the equilibrium mean-field model.
14 pages, 6 figures; Accepted by Physical Review E
References in corpus (4)
- Evidence for a dynamic phase transition in [Co/Pt]_3 magnetic multilayers
- Dynamic phase transition in the two-dimensional kinetic Ising model in an oscillating field: Universality with respect to the stochastic dynamic
- Conjugate field and fluctuation-dissipation relation for the dynamic phase transition in the two-dimensional kinetic Ising model
- Dynamic phase transition in the three-dimensional kinetic Ising model in an oscillating field
Cited by in corpus (5)
- Fluctuations in a model ferromagnetic film driven by a slowly oscillating field with a constant bias
- Monte Carlo study of the two-dimensional kinetic Ising model under a nonantisymmetric magnetic field
- Dynamical response of the Ising model to the amplitude modulated time dependent magnetic field
- Dynamic Phase Transitions in Mean-Field Ginzburg-Landau Models: Conjugate Fields and Fourier-Mode Scaling
- A comparative review of recent results on supercritical anomalies in two-dimensional kinetic Ising and Blume-Capel ferromagnets