Bekenstein-Hawking Entropy and Strange Metals

preprint2015arXivOpen access

Abstract

We examine models of fermions with infinite-range interactions which realize non-Fermi liquids with a continuously variable U(1) charge density Q\mathcal{Q}, and a non-zero entropy density S\mathcal{S} at vanishing temperature. Real time correlators of operators carrying U(1) charge qq at a low temperature TT are characterized by a Q\mathcal{Q}-dependent frequency ωS=(q T/ℏ)(∂S/∂Q)ω_{\mathcal{S}} = (q \, T/\hbar) (\partial \mathcal{S}/\partial{\mathcal{Q}}) which determines a spectral asymmetry. We show that the correlators match precisely with those of the AdS2_2 horizons of extremal charged black holes. On the black hole side, the matching employs S\mathcal{S} as the Bekenstein-Hawking entropy density, and the laws of black hole thermodynamics which relate (∂S/∂Q)/(2π)(\partial{\mathcal{S}}/\partial{\mathcal{Q}})/(2 π) to the electric field strength in AdS2_2. The fermion model entropy is computed using the microscopic degrees of freedom of a UV complete theory without supersymmetry.

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