Abstract
The description of the spin-glass phase in terms of a fixed point is shown to imply a "chaotic" phase in which the relative orientations of spins with large separations are sensitive to small changes in the temperature or in the bond strengths, where or , respectively, , and and are the thermal eigenvalue at the fixed point and the "interfacial (fractal) dimension," respectively.
- Received 20 October 1986
DOI:https://doi.org/10.1103/PhysRevLett.58.57
©1987 American Physical Society