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首页> 外文期刊>Modern Physics Letters, B. Condensed Matter Physics, Statistical Physics, Applied Physics >MAGNETIZATION IN ULTRATHIN FILMS - CRITICAL EXPONENT BETA FOR THE 2D XY MODEL WITH 4-FOLD CRYSTAL FIELDS
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MAGNETIZATION IN ULTRATHIN FILMS - CRITICAL EXPONENT BETA FOR THE 2D XY MODEL WITH 4-FOLD CRYSTAL FIELDS

机译:超薄膜的磁化-具有4折晶体场的二维XY模型的临界指数Beta

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摘要

Ultrathin XY-like magnetic films with 4-fold symmetry breaking crystal fields h(4) show a universal magnetization exponent beta approximate to 0.23. This suggests that the films fall into the universality class of the isotropic XY model, which we have proposed to be characterized, in any large but finite system, by an effective exponent beta = 3 pi(2)/128 approximate to 0.23. This empirical conclusion is at first sight in disagreement with theoretical expectations, which would place the films in a class of nonuniversal critical behavior characteristic of h(4), with beta = J/8h(4) much greater than 1. However, as h(4) is a marginal perturbation to the 2D-XY model, crossover to critical behavior characteristic of the perturbation occurs only after rescaling to an exponentially large length scale. We argue that this is the reason for the fact that the nonuniversal behavior characteristic of the crystal fields has not yet been observed in experiment. We present Monte Carlo data to show that one should always observe the universal magnetization characteristic of the finite size 2D-XY model, although there is a possibility of observing a crossover to non-power lau behavior characteristic of he at low temperature. [References: 38]
机译:具有4个对称打破晶体场h(4)的超薄XY样磁性膜显示通用磁化指数β约为0.23。这表明这些薄膜属于各向同性XY模型的通用性类别,在任何大型但有限的系统中,我们都建议用有效指数beta = 3 pi(2)/ 128近似于0.23来表征这些薄膜。乍看之下,这一经验结论与理论预期不一致,后者会使影片处于h(4)的一类非普遍临界行为特征,其中beta = J / 8h(4)远大于1。但是,当h (4)是2D-XY模型的边际扰动,扰动的临界行为特征只有在重新缩放为指数级的大尺度后才会发生变化。我们认为这是由于尚未在实验中观察到晶体场的普遍行为特征的原因。我们提出了蒙特卡洛数据,以表明人们应该始终观察有限尺寸2D-XY模型的通用磁化特性,尽管有可能观察到他在低温下与非功率Lau行为特性的交叉。 [参考:38]

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