The stiffness exponents in the glass phase for lattice spin glasses in dimensions d = 3, . . . , 6 are determined. To this end, we consider bond-diluted lattices near the T = 0 glass transition point p∗. This transition for discrete bond distributions occurs just above the bond percolation point pc in each dimension. Numerics suggests that both points, pc and p ∗, seem to share the same 1/d-expansion, at least for several leading orders, each starting with 1/(2d). Hence, these lattice graphs… CONTINUE READING