Phase transition dynamics in the three-dimensional field-free $\pm J$ Ising model
By using frustration-preserving hard-spin mean-field theory, we investigated the phase transition dynamics in the three-dimensional field-free $\pm J$ Ising spin glass model. As the temperature $T$ is decreased from paramagnetic phase at high temperatures, with a rate $ω=-dT/dt$ in time $t$, the critical temperature depends on the cooling rate through a clear power-law $ω^a$. With increasing antiferromagnetic bond fraction $p$, the exponent $a$ increases for the transition into the ferromagnetic case for $p p_\text{c}$, signaling the ferromagnetic-spin glass phase transition at $p_\text{c}\approx0.22$. The relaxation time is also investigated, at adiabatic case $ω=0$, and it is found that the dynamic exponent $zν$ increases with increasing $p$.