We study the overlap of two different eigenfunctions as compared with
self-overlap in the framework of an infinite-dimensional version of th
e disordered tight-binding model. Despite a very sparse structure of t
he eigenstates in the vicinity of the Anderson transition, their mutua
l overlap is still found to be of the same order as self-overlap as lo
ng as the energy separation is smaller than a critical value. The latt
er fact explains the robustness of the Wigner-Dyson level statistics e
verywhere in the phase of extended states. The same picture is expecte
d to hold for usual d-dimensional conductors, ensuring the s(beta) for
m of the level repulsion at a critical point.