Abstract
A Monte Carlo simulation of the two-dimensional random (±J) Ising model has characterized the equilibrium and dynamic behavior of the model. The spin-glass correlation length diverges algebraically with absolute temperature. The equilibration time obeys an Arrhenius law at low temperature. There is a "phase transition at zero temperature" and a glass transition at finite temperature. In the spin-glass frequency (f) regime the noise power spectrum is proportional to 1f(1+α) with α=0.28.

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