Critical Point Scaling of Ising Spin Glasses in a Magnetic Field
arXiv:1412.2448 · doi:10.1103/PhysRevB.91.104432
Abstract
Critical point scaling in a field applies for the limits , (where ) and but with the ratio finite. is a critical exponent of the zero-field transition. We study the replicon correlation length and from it the crossover scaling function defined via . We have calculated analytically for the mean-field limit of the Sherrington-Kirkpatrick model. In dimension d=3 we have determined the exponents and the critical scaling function within two versions of the Migdal-Kadanoff (MK) renormalization group procedure. One of the MK versions gives results for in d=3 in reasonable agreement with those of the Monte Carlo simulations at the values of R for which they can be compared. If there were a de Almeida-Thouless (AT) line for it would appear as a zero of the function at some negative value of R, but there is no evidence for such behavior. This is consistent with the arguments that there should be no AT line for , which we review.
9 pages, 8 figures
References in corpus (6)
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Cited by in corpus (7)
- The droplet-scaling versus replica symmetry breaking debate in spin glasses revisited
- Spin-glass dynamics: experiment, theory and simulation
- Evidence that the AT transition disappears below six dimensions
- Evidence of a second-order phase transition in the six-dimensional Ising spin glass in a field
- Comment on "Critical point scaling of Ising spin glasses in a magnetic field" by J. Yeo and M.A. Moore
- Reply to "Comment on "Critical Point Scaling of Ising Spin Glasses in a Magnetic Field" "
- Evidence of de Almeida-Thouless line below six dimensions