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自旋玻璃中的非微扰效应。

Non-perturbative effects in spin glasses.

作者信息

Castellana Michele, Parisi Giorgio

机构信息

Joseph Henry Laboratories of Physics and Lewis-Sigler Institute for Integrative Genomics, Princeton University, Princeton, New Jersey 08544, United States.

Dipartimento di Fisica, Università Sapienza, Rome, Italy.

出版信息

Sci Rep. 2015 Mar 3;5:8697. doi: 10.1038/srep08697.

DOI:10.1038/srep08697
PMID:25733337
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4346828/
Abstract

We present a numerical study of an Ising spin glass with hierarchical interactions--the hierarchical Edwards-Anderson model with an external magnetic field (HEA). We study the model with Monte Carlo (MC) simulations in the mean-field (MF) and non-mean-field (NMF) regions corresponding to d ≥ 4 and d < 4 for the d-dimensional ferromagnetic Ising model respectively. We compare the MC results with those of a renormalization-group (RG) study where the critical fixed point is treated as a perturbation of the MF one, along the same lines as in the -expansion for the Ising model. The MC and the RG method agree in the MF region, predicting the existence of a transition and compatible values of the critical exponents. Conversely, the two approaches markedly disagree in the NMF case, where the MC data indicates a transition, while the RG analysis predicts that no perturbative critical fixed point exists. Also, the MC estimate of the critical exponent ν in the NMF region is about twice as large as its classical value, even if the analog of the system dimension is within only ~2% from its upper-critical-dimension value. Taken together, these results indicate that the transition in the NMF region is governed by strong non-perturbative effects.

摘要

我们对具有层次相互作用的伊辛自旋玻璃——带外磁场的层次爱德华兹 - 安德森模型(HEA)进行了数值研究。我们分别在与(d)维铁磁伊辛模型中(d\geq4)和(d\lt4)相对应的平均场(MF)和非平均场(NMF)区域,用蒙特卡罗(MC)模拟研究该模型。我们将MC结果与重整化群(RG)研究的结果进行比较,在RG研究中,临界不动点被视为MF不动点的微扰,这与伊辛模型的(\epsilon)展开中的做法相同。MC和RG方法在MF区域结果一致,预测了相变的存在以及临界指数的兼容值。相反,在NMF情况下,这两种方法明显不同,MC数据表明存在相变,而RG分析预测不存在微扰临界不动点。此外,即使系统维度的类似值仅比其上临界维度值小约2%,NMF区域中临界指数(\nu)的MC估计值也约为其经典值的两倍。综合来看,这些结果表明NMF区域中的相变受强非微扰效应支配。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/8d251bc1ff3f/srep08697-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/e91eec360212/srep08697-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/44482e3f667b/srep08697-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/ea3a98e49b4c/srep08697-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/ce83afa03519/srep08697-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/c76317707c9e/srep08697-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/8d251bc1ff3f/srep08697-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/e91eec360212/srep08697-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/44482e3f667b/srep08697-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/ea3a98e49b4c/srep08697-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/ce83afa03519/srep08697-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/c76317707c9e/srep08697-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f4fb/4346828/8d251bc1ff3f/srep08697-f6.jpg

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