论文标题
结构无序磁铁的有效和渐近症
Effective and asymptotic criticality of structurally disordered magnets
论文作者
论文摘要
在实验和MC模拟中,通过由磁性和非磁性组件组成的稀释系统在实验中和MC模拟中通常举例说明了猝灭结构降低的磁体的磁临界行为的变化。通过我们的研究,我们的目的是表明,不仅可以观察到具有非磁杂质的稀释磁铁,而且可以通过存在两个(以及更多)化学上不同的磁性成分来实现的稀释磁铁。为此,我们考虑了一个结构排列的淬火磁铁的模型,其中所有晶格位点都被不同的长度$ l $的Ising样旋转所占据。在这样的随机自旋长度ISING模型中,每个自旋的长度$ l $是由分布函数$ p(l)$控制的随机变量。我们表明,该模型属于现场删除的ISING模型的通用类别。这证明了这两个模型都用相同的渐近临界指数值描述。但是,它们的有效批判行为有所不同。作为一个案例研究,我们考虑了两个不同磁铁的淬灭混合物,具有基本磁矩的值$ l_1 = 1 $和$ l_2 = s $,以及浓度$ c $和$ 1-c $,相应地。我们采用现场理论重新归一化组方法来分析不同初始条件的重新归一化组流量,该条件由$ s $和$ c $触发,并计算出远离重新归一化组转换的固定点的有效关键指数。我们展示了有效指数如何受磁成分性能差异的控制。
Changes in magnetic critical behaviour of quenched structurally-disordered magnets are usually exemplified in experiments and in MC simulations by diluted systems consisting of magnetic and non-magnetic components. By our study we aim to show, that similar effects can be observed not only for diluted magnets with non-magnetic impurities, but may be implemented, e.g., by presence of two (and more) chemically different magnetic components as well. To this end, we consider a model of the structurally-disordered quenched magnet where all lattice sites are occupied by Ising-like spins of different length $L$. In such random spin length Ising model the length $L$ of each spin is a random variable governed by the distribution function $p(L)$. We show that this model belongs to the universality class of the site-diluted Ising model. This proves that both models are described by the same values of asymptotic critical exponents. However, their effective critical behaviour differs. As a case study we consider a quenched mixture of two different magnets, with values of elementary magnetic moments $L_1=1$ and $L_2=s$, and of concentration $c$ and $1-c$, correspondingly. We apply field-theoretical renormalization group approach to analyze the renormalization group flow for different initial conditions, triggered by $s$ and $c$, and to calculate effective critical exponents further away from the fixed points of the renormalization group transformation. We show how the effective exponents are governed by difference in properties of the magnetic components.