Jang Hyunbum, Grimson Malcolm J, Woolf Thomas B
Department of Physiology, Johns Hopkins University, Baltimore, Maryland 21205, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2004 Oct;70(4 Pt 2):047101. doi: 10.1103/PhysRevE.70.047101. Epub 2004 Oct 5.
The dynamic phase behavior of a classical Heisenberg spin system with a bilinear exchange anisotropy in a planar thin film geometry has been investigated by Monte Carlo simulations using different forms for the stochastic dynamics. In simulations of the dynamic phase transition (DPT) in films subject to a pulsed oscillatory external field with competing surface fields, both Glauber and Metropolis dynamics show a continuous DPT. But while the field amplitude dependence of the DPT is similar in both cases, the transition region for the DPT as a function of temperature is more extended with Metropolis dynamics. The difference arises from a decoupling of the surface and bulk responses of the film near the dynamic phase transition with Metropolis dynamics that is not evident for Glauber dynamics.
利用不同形式的随机动力学,通过蒙特卡罗模拟研究了平面薄膜几何结构中具有双线性交换各向异性的经典海森堡自旋系统的动态相行为。在对受脉冲振荡外场和竞争表面场作用的薄膜中的动态相变(DPT)进行模拟时,格劳伯动力学和梅特罗波利斯动力学均显示出连续的DPT。但是,尽管两种情况下DPT的场振幅依赖性相似,但对于梅特罗波利斯动力学,DPT作为温度函数的转变区域更宽。这种差异源于在动态相变附近薄膜的表面和体响应的解耦,对于梅特罗波利斯动力学而言这种解耦是明显的,而对于格劳伯动力学则不明显。