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Seeing a c-theorem with holography

Robert C. Myers, Aninda Sinha

Abstract

There is no known model in holography exhibiting a $c$-theorem where the central charges of the dual CFT are distinct. We examine a holographic model of RG flows in a framework where the bulk gravity theory contains higher curvature terms. The latter allows us to distinguish the flow of the central charges $a$ and $c$ in the dual field theories in four dimensions. One finds that the flow of $a$ is naturally monotonic but that of $c$ is not. Extending the analysis of holographic RG flows to higher dimensions, we are led to formulate a novel c-theorem in arbitrary dimensions for a universal coefficient appearing in the entanglement entropy of the fixed point CFT's.

Seeing a c-theorem with holography

Abstract

There is no known model in holography exhibiting a -theorem where the central charges of the dual CFT are distinct. We examine a holographic model of RG flows in a framework where the bulk gravity theory contains higher curvature terms. The latter allows us to distinguish the flow of the central charges and in the dual field theories in four dimensions. One finds that the flow of is naturally monotonic but that of is not. Extending the analysis of holographic RG flows to higher dimensions, we are led to formulate a novel c-theorem in arbitrary dimensions for a universal coefficient appearing in the entanglement entropy of the fixed point CFT's.

Paper Structure

This paper contains 20 equations, 1 figure.

Figures (1)

  • Figure 1: A slice of constant $t$ through the AdS$_{d+1}$ metric in eq. (\ref{['metric1']}). This slice bears some similarity to the Einstein-Rosen bridge in a Schwarzschild black hole HE. Note that only half of the AdS boundary is reached in the limit $r\rightarrow\infty$. The other half is reached from the second asymptotic region 'behind the horizon'.