Abstract

We use Euclidean path integrals to explore the set of bulk asymptotically AdS spacetimes with good CFT duals. We consider simple bottom-up models of bulk physics defined by Einstein-Hilbert gravity coupled to thin domain walls and restrict to solutions with spherical symmetry. The cosmological constant is allowed to change across the domain wall, modeling more complicated Einstein-scalar systems where the scalar potential has multiple minima. In particular, the cosmological constant can become positive in the interior. However, in the above context, we show that inflating bubbles are never produced by smooth Euclidean saddles to asymptotically AdS path integrals. The obstacle is a direct parallel to the well-known obstruction to creating inflating universes by tunneling from flat space. In contrast, we do find good saddles that create so-called “bag-of-gold” geometries which, in addition to their single asymptotic region, also have an additional large semi-classical region located behind both past and future event horizons. Furthermore, without fine-tuning model parameters, using multiple domain walls we find Euclidean geometries that create arbitrarily large bags-of-gold inside a black hole of fixed horizon size, and thus at fixed Bekenstein-Hawking entropy. Indeed, with our symmetries and in our class of models, such solutions provide the unique semi-classical saddle for appropriately designed (microcanonical) path integrals. This strengthens a classic tension between such spacetimes and the CFT density of states, similar to that in the black hole information problem.

Highlights

  • AdSSchwarzschild region exterior attached to an interior that is essentially an large Friedman-Lemaıtre-RobertsonWalker (FLRW) cosmology, which we take here to be filled with whatever bulk radiation is natural in the theory;1 see figure 1

  • For solutions with a single domain wall of the sort we have studied far, the size of a bag-of-gold is largely dictated by rmin, which from (2.1) is the maximum radius of any SD−2 of spherical symmetry inside the black hole

  • We could construct an arbitrarily large bag-of-gold by chaining together many copies of the same fundamental unit consisting of an Schwarzschild anti-de Sitter (SAdS) region like that shown at fight in figure 11, bounded on each side by identical domain walls, with each wall described in the formalism of section 2 by setting μi = μe = μ

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Summary

Thin wall spacetimes in AdS

Our domain walls will separate two vacua which we call interior and exterior. Our focus will be on cases in which the exterior solution extends to an asymptotically AdS boundary, and in particular where it does so on the moment of time symmetry (t = 0). Since our solutions will be constructed by cutting and pasting pieces of the exterior and interior metrics specified by (2.2), it will be useful to directly find the curves defined by the domain wall in both the (r, te) and (r,ti) planes. We make explicit that the interior and exterior generically define two different time coordinates tEi, tEe along the wall as the coordinates of (2.1) are not guaranteed to be continuous at the domain wall.

No AlAdS spacetimes with inflating interiors
No other inflating cases in stable theories
Good saddles are non-degenerate
Comments on self-intersecting walls
Non-inflating interiors
Creating bags of gold
External solutions without self-intersections
Euclidean wormholes and large bags of gold from multiple domain walls
Can Euclidean wormholes and large bags of gold dominate a path integral?
Discussion
Findings
C Constraints on the size of single-wall bags of gold
Full Text
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