Abstract
The hysteresis loop in the zero-temperature random-field Ising model exhibits a critical point as the width of the disorder increases. Above six dimensions, the critical exponents of this transition, where the ‘‘infinite avalanche’’ first disappears, are described by mean-field theory. We expand the critical exponents about mean-field theory, in 6-ε dimensions, to first order in ε. Despite ε=3, the values obtained agree reasonably well with the numerical values in three dimensions.
- Received 16 July 1993
DOI:https://doi.org/10.1103/PhysRevLett.71.3222
©1993 American Physical Society