  The time-dependent susceptibility for the finite-size mean-field Random
Orthogonal model (ROM) is studied numerically for temperatures above the
mode-coupling temperature. The results show that the imaginary part of the
susceptibility $\chi''(\nu)$ obeys the scaling form proposed for glass-forming
liquids with the peak frequency decreasesing as the temperature is lowered
consistently with the Vogel-Fulcher law with a critical temperature remarkably
close to the known critical temperature $T_c$ of the model where the
configurational entropy vanishes.
