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We have computed the time-dependent susceptibility for the finite-size mean-field Random Orthogonal model (ROM). We find that for temperatures above the mode-coupling temperature the imaginary part of the susceptibility obeys the scaling forms proposed for glass-forming liquids. Furthermore, as the temperature is lowered the peak frequency of decreases following a Vogel-Fulcher law with a critical temperature remarkably close to the known critical temperature where the configurational entropy vanishes.

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