LANDAU THEORY OF QUANTUM SPIN-GLASSES OF ROTORS AND ISING SPINS

被引:143
作者
READ, N
SACHDEV, S
YE, J
机构
[1] YALE UNIV,DEPT APPL PHYS,NEW HAVEN,CT 06520
[2] HARVARD UNIV,DEPT PHYS,CAMBRIDGE,MA 02138
来源
PHYSICAL REVIEW B | 1995年 / 52卷 / 01期
基金
美国国家科学基金会;
关键词
D O I
10.1103/PhysRevB.52.384
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We consider quantum rotors or Ising spins in a transverse field on a d-dimensional lattice, with random, frustrating, short-range, exchange interactions. The quantum dynamics are associated with a finite moment of inertia for the rotors, and with the transverse field for the Ising spins. For a suitable distribution of exchange constants, these models display spin-glass and quantum paramagnet phases and a zero-temperature (T) quantum transition between them. An earlier exact solution for the critical properties of a model with infinite-range interactions cna be reproduced by minimization of a Landau effective-action functional for the model in finite d with short-range interactions. The functional is expressed in terms of a composite spin field which is bilocal in time. The mean-field phase diagram near the T=0 critical point is mapped out as a function of T, strength of the quantum coupling, and applied fields. The spin-glass phase has replica symmetry breaking; but, as in the classical Ising spin glass, the order parameter becomes replica symmetric as T0. Next we examine the consequences of fluctuations about the mean field for the critical properties. Above d=8, and with certain restrictions on the values of the Landau couplings, we find that the transition is controlled by a Gaussian fixed point with mean-field critical exponents. For couplings not attracted by the Gaussian fixed point above d=8, and for all physical couplings below d=8, we find runaway renormalization-group flows to strong coupling. General scaling relations that should be valid even at the strong-coupling fixed point are proposed and compared with Monte Carlo simulations. © 1995 The American Physical Society.
引用
收藏
页码:384 / 410
页数:27
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