Thermodynamic Chaos and the Structure of Short-Range Spin Glasses

This paper presents an approach, recently introduced by the authors and based on the notion of “metastates,” to the chaotic size dependence expected in systems with many competing pure states and applies it to the Edwards-Anderson (EA) spin glass model. We begin by reviewing the standard picture of the EA model based on the Sherrington-Kirkpatrick (SK) model and why that standard SK picture is untenable. Then we introduce metastates, which are the analogues of the invariant probability measures describing chaotic dynamical systems and discuss how they should appear in several models simpler than the EA spin glass. Finally, we consider possibilities for the nature of the EA metastate, including one which is a nonstandard SK picture, and speculate on their prospects. An appendix contains proofs used in our construction of metastates and in the earlier construction by Aizenman and Wehr.

[1]  Exotic states in long-range spin glasses , 1993 .

[2]  Charles M. Newman,et al.  The stochastic geometry of invasion percolation , 1985 .

[3]  A. Young,et al.  Role of initial conditions in spin glass dynamics and significance of Parisi's q(x) , 1983 .

[4]  J. Fröhlich,et al.  The high-temperature phase of long-range spin glasses , 1987 .

[5]  Maritan,et al.  Optimal paths and domain walls in the strong disorder limit. , 1994, Physical review letters.

[6]  T. D. Lee,et al.  Statistical Theory of Equations of State and Phase Transitions. II. Lattice Gas and Ising Model , 1952 .

[7]  T. D. Lee,et al.  Statistical Theory of Equations of State and Phase Transitions. I. Theory of Condensation , 1952 .

[8]  Geoffrey Grimmett,et al.  Probability and Phase Transition , 1994 .

[9]  M. A. Virasoro,et al.  Random free energies in spin glasses , 1985 .

[10]  J. Rehr,et al.  High-temperature series for scalar-field Lattice models: Generation and analysis , 1990 .

[11]  J. Bricmont,et al.  Phase transition in the 3d random field Ising model , 1988 .

[12]  Giorgio Parisi,et al.  Order parameter for spin-glasses , 1983 .

[13]  J. Fröhlich,et al.  Absence of symmetry breaking forN-vector spin glass models in two dimensions , 1985 .

[14]  D. Huse,et al.  Pure states in spin glasses , 1987 .

[15]  Sample to sample fluctuations in the random energy model , 1985 .

[16]  F. Ledrappier Pressure and variational principle for random Ising model , 1977 .

[17]  M. Mézard,et al.  Spin Glass Theory and Beyond , 1987 .

[18]  A. E. Patrick,et al.  Random infinite-volume Gibbs states for the Curie-Weiss random field Ising model , 1992 .

[19]  J. Imbrie The ground state of the three-dimensional random-field Ising model , 1985 .

[20]  J. Fröhlich,et al.  A heuristic theory of the spin glass phase , 1986 .

[21]  Stiffness exponent, number of pure states, and Almeida-Thouless line in spin-glasses , 1990 .

[22]  F. Papangelou GIBBS MEASURES AND PHASE TRANSITIONS (de Gruyter Studies in Mathematics 9) , 1990 .

[23]  Charles M. Newman,et al.  Topics in Disordered Systems , 1997 .

[24]  Leonid Pastur,et al.  Absence of self-averaging of the order parameter in the Sherrington-Kirkpatrick model , 1991 .

[25]  S. Edwards,et al.  Theory of spin glasses , 1975 .

[26]  Hans-Otto Georgii,et al.  Gibbs Measures and Phase Transitions , 1988 .

[27]  S. Kirkpatrick,et al.  Solvable Model of a Spin-Glass , 1975 .

[28]  Fisher,et al.  Equilibrium behavior of the spin-glass ordered phase. , 1988, Physical review. B, Condensed matter.

[29]  Timo Seppäläinen,et al.  Entropy, limit theorems, and variational principles for disordered lattice systems , 1995 .

[30]  Francis Comets,et al.  Large deviation estimates for a conditional probability distribution. Applications to random interaction Gibbs measures , 1989 .

[31]  Moore,et al.  Chaotic nature of the spin-glass phase. , 1987, Physical review letters.

[32]  Ground-state structure in a highly disordered spin-glass model , 1995, adap-org/9505005.

[33]  Newman,et al.  Non-mean-field behavior of realistic spin glasses. , 1996, Physical review letters.

[34]  J. Bouchaud Weak ergodicity breaking and aging in disordered systems , 1992 .

[35]  C. Newman,et al.  Uniqueness of the infinite component in a random graph with applications to percolation and spin glasses , 1992 .

[36]  Michael Aizenman,et al.  Translation invariance and instability of phase coexistence in the two dimensional Ising system , 1980 .

[37]  Fisher,et al.  Ordered phase of short-range Ising spin-glasses. , 1986, Physical review letters.

[38]  L. Onsager Crystal statistics. I. A two-dimensional model with an order-disorder transition , 1944 .

[39]  E. Olivieri,et al.  One dimensional spin glasses with potential decay 1/r1+g. Absence of phase transitions and cluster properties , 1987 .

[40]  W. L. Mcmillan Scaling theory of Ising spin glasses , 1984 .

[41]  Michael Aizenman,et al.  Rounding effects of quenched randomness on first-order phase transitions , 1990 .

[42]  Newman,et al.  Multiple states and thermodynamic limits in short-ranged Ising spin-glass models. , 1992, Physical review. B, Condensed matter.

[43]  Giorgio Parisi,et al.  Infinite Number of Order Parameters for Spin-Glasses , 1979 .

[44]  M. Mézard,et al.  Nature of the Spin-Glass Phase , 1984 .

[45]  Robijn Bruinsma,et al.  Soft order in physical systems , 1994 .

[46]  C. Newman Disordered Ising Systems and Random Cluster Representations , 1994 .

[47]  Newman,et al.  Spatial inhomogeneity and thermodynamic chaos. , 1995, Physical Review Letters.

[48]  Newman,et al.  Spin-glass model with dimension-dependent ground state multiplicity. , 1994, Physical review letters.

[49]  B. Simon,et al.  Infrared bounds, phase transitions and continuous symmetry breaking , 1976 .

[50]  van Aernout Enter,et al.  Overlap distributions for deterministic systems with many pure states , 1992 .