Abstract

According to Witten [1], the conformal boundary condition of gravity, which specifies the conformal geometry of the boundary and the trace of the extrinsic curvature, is elliptic and leads to well-defined perturbation theory of gravity about any classical solution. The conformal boundary condition was previously considered in [2, 3] in the context of AdS/BCFT, wherein the equation of motion of the end-of-the-world was derived and emphasized. In this paper, we investigate further other consequences of the conformal boundary condition in AdS/BCFT. We derive the boundary central charges of the holographic Weyl anomaly and show that they are exactly the same for conformal boundary condition and Dirichlet boundary condition. We analysis the metric perturbation with conformal boundary condition (CBC), Dirichlet boundary condition (DBC) and Neumann boundary condition (NBC) imposed on the end-of-the-world brane and show that they admit an interpretation as the fluctuation of the extrinsic curvature (case of CBC and DBC) and the induced metric (case of NBC) of Q respectively. In all cases, the fluctuation modes are massive, which are closely relevant to the massive island formation in the literature. Our results reveal that there are non-trivial gravitational dynamics from extrinsic curvatures on the conformal and Dirichlet branes, which may have interesting applications to the island. We also discuss, in passing, the localization of gravitons in brane world theory. We find that, contrary to NBC, the graviton for CBC/DBC is located on the brane with non-positive tension instead of non-negative tension.

Highlights

  • Has been proposed [45, 46]

  • We analysis the metric perturbation with conformal boundary condition (CBC), Dirichlet boundary condition (DBC) and Neumann boundary condition (NBC) imposed on the end-of-the-world brane and show that they admit an interpretation as the fluctuation of the extrinsic curvature and the induced metric of Q respectively

  • We argue that CBC/DBC and NBC all define a consistent theory of AdS/BCFT

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Summary

Metric perturbations for different BCs

According to [35], CBC is elliptic and leads to a well-defined perturbation theory for gravity. We analysis the metric perturbation with CBC, DBC and NBC imposed respectively on the end-of-the-world brane Q. Our results below for the spectrum of gravitons is independent of the choice of the unperturbed metric. Note that DBC yields the same condition (5.10). This implies that the spectrum of fluctuations are the same for CBC and DBC. Each mode of fluctuation of h(ij1) represents a massive graviton of mass m in the theory. It has the interpretation as fluctuation mode δKij = − 2 cosh2(ρ)H (−ρ)h(ij). Note that the perturbation (5.12), while nontrivial, keeps K invariant and this is consistent with the CBC and DBC

Mass spectrum
Two point functions in BCFT
Relation to massive island
Conclusions
B Mass spectrum for massive bulk scalar field
C Localization of gravity
Volcanic potential
Wave function

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