Abstract
We study the vacuum correlations of a gravitational field in any dimension N>2 using the perturbative expansion to order G. It is known that the usual Green's functions are meaningless in quantum gravity; moreover, we show that the traces of the holonomies of the Christoffel connection vanish, revealing a striking difference between gravity and Yang-Mills theories. In order to define meaningful holonomies we make two physical requirements: (1) the contours of the loop integrals must have "geodesic form and size;" (2) the full rotation matrices, not just their traces, must be averaged. Following these ideas we compute a "dumbbell correlation function" which turns out to behave like GDN+2, where D is the geodesic distance. Finally, we write a gauge-invariant quantity which could replace the Wilson loop in reproducing the static potential energy between two sources.