Abstract
We consider phase transitions in systems where the field conjugate to the order parameter is static and random. It is demonstrated that when the order parameter has a continuous symmetry, the ordered state is unstable against an arbitrarily weak random field in less than four dimensions. The borderline dimensionality above which mean-field-theory results hold is six.
- Received 12 August 1975
DOI:https://doi.org/10.1103/PhysRevLett.35.1399
©1975 American Physical Society