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arXiv 1111.3468cond-mat.dis-nn
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$d=2,3$维随机横场伊辛模型:通过非线性传递方法的无限无序标度

Random Transverse Field Ising Model in dimension $d=2,3$ : Infinite Disorder scaling via a non-linear transfer approach

Cecile Monthus, Thomas Garel

摘要:

对Cayley树上的随机横场伊辛模型发展了“腔平均场”近似[L. Ioffe和M. Mézard,PRL 105,037001(2010)]已被发现再现$d=1$ [0. Dimitrova和M. Mézard,J. Stat. Mech.(2011)P01020]。在本文中,我们建议通过非线性转移方法的表面磁化在有限维$d>1$扩展这些想法。在无序相,转移方程的线性化对应于横向尺寸为$D=d-1$的随机介质中定向聚合物的转移矩阵,与首阶微扰标度分析一致[C. Monthus和T. Garel,arxiv:1110.3145]。我们提出的非线性传输方法在尺寸$d=2$和$d=3$的数值结果。在这两种情况下,我们发现临界点是由无限无序标度。特别是在临界状态下,一点表面磁化强度按比例缩放为$\ln m_L^{surf} \simeq - L^{ω_c} v$,其中$ω_c(d)$与相应定向聚合物模型的液滴指数$ω_{DP}(D=d-1)$一致,其中$ω_c(d=2)=1/3$和$ω_c(d=3) \simeq 0.24$。O(1)阶正随机变量$v$的分布$P(v)$在原点$P(v) \propto v^a$和$a(d=2,3)>0$附近呈现幂律奇异性,因此表面磁化强度的所有时刻都由相同的幂律衰减$\bar{(m_L^{surf})^k} \propto L^{- x_S}$和$x_S=ω_c (1+a)$决定,与$k$阶无关。

英文摘要:

The 'Cavity-Mean-Field' approximation developed for the Random Transverse Field Ising Model on the Cayley tree [L. Ioffe and M. Mézard, PRL 105, 037001 (2010)] has been found to reproduce the known exact result for the surface magnetization in $d=1$ [O. Dimitrova and M. Mézard, J. Stat. Mech. (2011) P01020]. In the present paper, we propose to extend these ideas in finite dimensions $d>1$ via a non-linear transfer approach for the surface magnetization. In the disordered phase, the linearization of the transfer equations correspond to the transfer matrix for a Directed Polymer in a random medium of transverse dimension $D=d-1$, in agreement with the leading order perturbative scaling analysis [C. Monthus and T. Garel, arxiv:1110.3145]. We present numerical results of the non-linear transfer approach in dimensions $d=2$ and $d=3$. In both cases, we find that the critical point is governed by Infinite Disorder scaling. In particular exactly at criticality, the one-point surface magnetization scales as $\ln m_L^{surf} \simeq - L^{ω_c} v$, where $ω_c(d)$ coincides with the droplet exponent $ω_{DP}(D=d-1)$ of the corresponding Directed Polymer model, with $ω_c(d=2)=1/3$ and $ω_c(d=3) \simeq 0.24$. The distribution $P(v)$ of the positive random variable $v$ of order O(1) presents a power-law singularity near the origin $P(v) \propto v^a$ with $a(d=2,3)>0$ so that all moments of the surface magnetization are governed by the same power-law decay $\bar{(m_L^{surf})^k} \propto L^{- x_S}$ with $x_S=ω_c (1+a)$ independently of the order $k$.

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