Random field Ising model swept by propagating magnetic field wave: Athermal nonequilibrium phase diagram

TL;DR

This study uses Monte Carlo simulations to explore the nonequilibrium phases of a two-dimensional random field Ising model under a propagating magnetic wave, identifying four distinct steady states and mapping their phase diagram.

Contribution

It introduces a detailed phase diagram of the nonequilibrium steady states in a random field Ising model driven by a propagating magnetic wave at zero temperature.

Findings

Identified four distinct dynamical steady states.

Mapped phase diagram based on wave amplitude and random field strength.

Confirmed phases are robust, not finite size effects or transients.

Abstract

The dynamical steady state behaviour of the random field Ising ferromagnet swept by a propagating magnetic field wave is studied at zero temperature by Monte Carlo simulation in two dimensions. The distribution of the random field is bimodal type. For a fixed set of values of the frequency and wavelength of propagating magnetic field wave and the strength of the random field, four distinct dynamical steady states or nonequilibrium phases were identified. These four nonequilibrium phases are characterised by different values of structure factors. State of first kind, where all spins are parallel (up). The second one is, the propagating type, where the sharp strips formed by parallel spins are found to move coherently. The third one is also propagating type, where the boundary of the strips of spins is not very sharp. The fourth kind, shows no propagation of stripes of magnetic spins, forming a homogeneous distribution of up and down spins. This is disordered phase The appearance of these four dynamical phases or modes depends on the value of the amplitude of propagating magnetic field wave and the strength of random (static) field. A phase diagram has also been drawn, in the plane formed by the amplitude of propagating field and the strength of random field. It is checked that, the existence of these dynamical phases is neither a finite size effect nor a transient phenomenon.