Abstract
Measurements are reported of the pressure dependence of the real part of the dielectric constant of subcritical and supercritical Hg vapor. Abrupt upward deviations from normal Clausius-Mosotti behavior, which are exhibited in an extremely narrow pressure range in the subcritical vapor phase, indicate that the vapor-liquid phase transition near the critical region is preceded by a heretofore undetected "plasma transition." It is concluded that the dielectric anomaly is caused by the formation of dense, charged thermodynamically stable droplets.