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Nonequilibrium Phase Transition in Spin-S Ising Ferromagnet Driven by Propagating and Standing Magnetic Field Wave

机译:通过传播和站立磁场波驱动的Spin-S ising铁磁性中的异频阶段过渡

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摘要

The dynamical response of spin-S (S= 1, 3/2, 2, 3) Ising ferromagnet to the plane propagating wave, standing magnetic field wave and uniformly oscillating field with constant frequency are studied separately in two dimensions by extensive Monte Carlo simulation. Depending upon the strength of the magnetic field and the value of the spin state of the Ising spin lattice two different dynamical phases are observed. For a fixed value of S and the amplitude of the propagating magnetic field wave the system undergoes a dynamical phase transition from propagating phase to pinned phase as the temperature of the system is cooled down. Similarly in case with standing magnetic wave the system undergoes dynamical phase transition from high temperature phase where spins oscillate coherently in alternate bands of half wavelength of the standing magnetic wave to the low temperature pinned or spin frozen phase. For a fixed value of the amplitude of magnetic field oscillation the transition temperature is observed to decrease to a limiting value as the value of spin S is increased. The time averaged magnetisation over a full cycle of the magnetic field oscillation plays the role of the dynamic order parameter. A comprehensive phase boundary is drawn in the plane of magnetic field amplitude and dynamic transition temperature. It is found that the phase boundary shrinks inwards for high value of spin state S. Also in the low temperature (and high field) region the phase boundaries are closely spaced.
机译:通过广泛的Monte Carlo仿真分别在两个维度中分别研究Spin-S(S = 1,3 / 2,2,3)的动态响应到平面传播波,常频,常量频率恒定的频率均匀振荡场。取决于磁场的强度和旋转晶格的旋转状态的值,观察到两种不同的动力相。对于S的固定值以及传播磁场的幅度波,系统经历从传播相位到固定相位的动态相位转变,因为系统的温度被冷却下来。类似地,在常设磁波的情况下,系统经历从高温阶段进行动态相变,其中旋转在站立磁波的半波长的交替条带中振荡到低温钉扎或旋转冷冻相。对于磁场振幅的固定值振荡,随着旋转S的值增加,观察到转变温度减小到限制值。在磁场振荡的完整周期上的时间平均磁化起到动态顺序参数的作用。在磁场幅度和动态转变温度的平面中绘制了综合相边界。发现相位边界在旋转状态S的高值向内收缩,在低温(和高场)区域中,相位边界是紧密间隔的。

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