Abstract

The data analysis procedures employed in our previous publications [Phys. Rev. A 45, 3867 (1992); 46, 3343 (1992); Phys. Rev. E 47, 4223 (1993)] are reviewed and the significance of the cusp found in the scaling time ${\mathrm{\ensuremath{\tau}}}_{\mathrm{\ensuremath{\beta}}}$ is described. The implications of the Salol dielectric susceptibility results described by Dixon, Menon, and Nagel in their Comment [preceding paper, Phys. Rev. E 50, 1717 (1994)] are discussed. The relation between the alternative model presented in the Comment by Zeng, Kivelson, and Tarjus [second preceding paper, Phys. Rev. E 50, 1711 (1994)] and the mode-coupling theory is considered, and their alternative model is shown to be incompatible with experimental results, particularly inelastic neutron-scattering spectroscopy where the dipole--induced-dipole scattering mechanism is inoperative.

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