Holographic renormalization conjecture for bulk Laplacian eigenvalue variation

Let (X,G)(X,G) be the bulk with boundary MM, and let D~=ΔG\tilde{D}=-\Delta_G and D=ΔgD=-\Delta_g be the bulk and boundary Laplace--Beltrami operators, respectively. Here λ\lambda is an eigenvalue of D~\tilde{D}, ρ\rho is the holographic renormalization parameter, and ζ(s,D)\zeta(s,D) is the spectral zeta function of DD. Holographic eigenvalue-variation conjecture. In the geometric setup of the AdS/CFT correspondence, holographic renormalization gives

λρ=12ζ(0,D)+ρζ(0,D).\frac{\partial \lambda}{\partial \rho}=-\frac{1}{2}\zeta'(0,D)+\rho\zeta(0,D).

In the first-term approximation, this becomes

λρ=12ζ(0,D).\frac{\partial \lambda}{\partial \rho}=-\frac{1}{2}\zeta'(0,D).

The claim connects spectral data of the boundary Laplacian with the variation of bulk eigenvalues and is motivated by the relation between thermal entropy, free energy, and holographic renormalization in odd-dimensional bulk geometry. The supplied text gives no evidence that the conjecture has been resolved.

Sources & referencesView supporting material

Primary source

Dan Li, “Renormalization group flow, Entropy and Eigenvalues”, arXiv:1604.01843 (2017).

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