Key points are not available for this paper at this time.
The three-dimensional random Ising model with a Gaussian distribution of nearest-neighbor interactions is studied for the pure spin-glass case where the average interaction vanishes. The distribution of domain-wall free energies at finite temperature is calculated with the use of the Metropolis Monte Carlo algorithm for finite lattices. A renormalization-group transformation is set up which preserves the domain-wall free-energy distribution when the lattice parameter is changed. The spin-glass transition temperature is found to be T₆= (1. 00. 2) J \~ where J \~ is the variance of the Gaussian interaction distribution. The thermal exponent is =1. 80. 5 and the heat-capacity exponent is =-3. 41. 5. The heat capacity exhibits a rounded peak at higher temperatures.
W. L. McMillan (Tue,) studied this question.