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We describe the interplay of quantum and thermal fluctuations in the infinite-range Heisenberg spin glass. This model is generalized to SU(N) symmetry, and we describe the phase diagram as a function of the spin S and temperature T. The model is solved in the large-N limit, and certain universal critical properties are shown to hold to all orders in $1/N.$ For large S, the ground state is a spin glass, but quantum effects are crucial in determining the low-T thermodynamics: we find a specific heat linear in T and a local spectral density of spin excitations, χloc^''(ω)~ω for a spin-glass state which is marginally stable to fluctuations in the replicon modes. For small S, the spin-glass order is fragile, and a spin-liquid state with χloc^''~tanh(ω/2T) dominates the properties over a significant range of T and {ω}. We argue that the latter state may be relevant in understanding the properties of strongly disordered transition-metal and rare-earth compounds.
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Georges et al. (2001) studied this question.
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