Janzen K, Engel A, Mézard M
Institut für Physik, Carl-von-Ossietsky Universität, Oldenburg, Germany.
Phys Rev E Stat Nonlin Soft Matter Phys. 2010 Aug;82(2 Pt 1):021127. doi: 10.1103/PhysRevE.82.021127. Epub 2010 Aug 30.
We investigate the Lévy glass, a mean-field spin-glass model with power-law distributed couplings characterized by a divergent second moment. By combining extensively many small couplings with a spare random backbone of strong bonds the model is intermediate between the Sherrington-Kirkpatrick and the Viana-Bray models. A truncated version where couplings smaller than some threshold ε are neglected can be studied within the cavity method developed for spin glasses on locally treelike random graphs. By performing the limit ε→0 in a well-defined way we calculate the thermodynamic functions within replica symmetry and determine the de Almeida-Thouless line in the presence of an external magnetic field. Contrary to previous findings we show that there is no replica-symmetric spin-glass phase. Moreover we determine the leading corrections to the ground-state energy within one-step replica symmetry breaking. The effects due to the breaking of replica symmetry appear to be small in accordance with the intuitive picture that a few strong bonds per spin reduce the degree of frustration in the system.
我们研究了列维玻璃,它是一种平均场自旋玻璃模型,其耦合具有幂律分布,特征是二阶矩发散。通过将大量小耦合与稀疏的强键随机主干相结合,该模型介于谢林顿 - 柯克帕特里克模型和维亚纳 - 布雷模型之间。对于耦合小于某个阈值ε的截断版本,可以在为局部树状随机图上的自旋玻璃开发的腔方法内进行研究。通过以明确的方式进行ε→0的极限运算,我们在复制对称内计算热力学函数,并确定存在外磁场时的德阿尔梅达 - 图勒斯线。与先前的发现相反,我们表明不存在复制对称自旋玻璃相。此外,我们在一步复制对称破缺内确定了基态能量的主要修正。根据每个自旋有一些强键会降低系统中受挫程度的直观图像,复制对称破缺引起的影响似乎很小。