We demonstrate the level statistics in the vicinity of the Anderson tr
ansition in d > 2 dimensions to be universal and drastically different
from both Wigner-Dyson in the metallic regime and Poisson in the insu
lator regime. The variance of the number of levels N in a given energy
interval with [N] >> 1 is proved to behave as (N)gamma where gamma =
1 - (nud)-1 and nu is the correlation length exponent. The inequality
gamma < 1, shown to be required by an exact sum rule, results from non
trivial cancellations (due to the causality and scaling requirements)
in calculating the two-level correlation function.