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We investigate the dissipative loss in the $\pm J$ Ising spin glass in threedimensions through the scaling of the hysteresis area, for a maximum magneticfield that is equal to the saturation field. We perform a systematic analysisfor the whole range of the bond randomness as a function of the sweep rate, bymeans of frustration-preserving hard-spin mean field theory. Data collapsewithin the entirety of the spin-glass phase driven adiabatically (i.e.,infinitely-slow field variation) is found, revealing a power-law scaling of thehysteresis area as a function of the antiferromagnetic bond fraction and thetemperature. Two dynamic regimes separated by a threshold frequency $\omega_c$characterize the dependence on the sweep rate of the oscillating field. For$\omega < \omega_c$, the hysteresis area is equal to its value in the adiabaticlimit $\omega = 0$, while for $\omega > \omega_c$ it increases with thefrequency through another randomness-dependent power law.

Deep Spin-Glass Hysteresis Area Collapse and Scaling in the $d=3$ $\pm J$ Ising Model