Scaling Analysis of Domain-Wall Free-Energy in the Edwards-Anderson Ising Spin Glass in a Magnetic Field
arXiv:cond-mat/0702302 · doi:10.1103/PhysRevLett.99.137202
Abstract
The stability of the spin-glass phase against a magnetic field is studied in the three and four dimensional Edwards-Anderson Ising spin glasses. Effective couplings and effective fields associated with length scale L are measured by a numerical domain-wall renormalization group method. The results obtained by scaling analysis of the data strongly indicate the existence of a crossover length beyond which the spin-glass order is destroyed by field H. The crossover length well obeys a power law of H which diverges as H goes to zero but remains finite for any non-zero H, implying that the spin-glass phase is absent even in an infinitesimal field. These results are well consistent with the droplet theory for short-range spin glasses.
4 pages, 5 figures; The text is slightly changed, the figures 3, 4 and 5 are changed, and a few references are added
References in corpus (2)
Cited by in corpus (5)
- Behavior of Ising Spin Glasses in a Magnetic Field
- Single-particle excitations under coexisting electron correlation and disorder: a numerical study of the Anderson-Hubbard model
- Evidence against a mean field description of short-range spin glasses revealed through thermal boundary conditions
- Effect of magnetoelastic coupling on spin-glass behavior in Heisenberg pyrochlore antiferromagnets with bond disorder
- First-order phase transition in a 2D random-field Ising model with conflicting dynamics