1993 年 62 巻 2 号 p. 435-438
The three-dimensional ±J Ising spin glass model is investigated by means of Monte Carlo simulation. In uniform fields of various strength, the Edwards-Anderson susceptibility χEAQ is calculated at T=0.9J which is lower than the transition temperature in the zero-field case. It is found that χEA decreases monotonically when the field strength is increased and that the data do not suggest a phase transition in a finite field. The best parameters for the scaling function of the form χEA(H)\simeqlψ\ ildeχEA((H−Hc)l−φ) are estimated to be Hc=0.00(10)J, ψ=2.16(22) and φ=−1.13(6). These results support the hypothesis that the phase transition does not exist in a finite magnetic field.
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