We evaluate the high temperature limit of the free energy of spin glasses on
the hypercube with Hamiltonian HN(σ)=σTJσ, where the
coupling matrix J is drawn from certain symmetric orthogonally invariant
ensembles. Our derivation relates the annealed free energy of these models to a
spherical integral, and expresses the limit of the free energy in terms of the
limiting spectral measure of the coupling matrix J. As an application, we
derive the limiting free energy of the Random Orthogonal Model (ROM) at high
temperatures, which confirms non-rigorous calculations of Marinari et al.
(1994). Our methods also apply to other well-known models of disordered
systems, including the SK and Gaussian Hopfield models.Comment: 15 pages, 1 figur