We explore asymptotically AdS 2 solutions of a particular two-dimensional dilaton-gravity theory. In the deep interior, these solutions flow to the cosmological horizon of dS 2 . We calculate various matter perturbations at the linearised and non-linear level. We consider both Euclidean and Lorentzian perturbations. The results can be used to characterise the features of a putative dual quantum mechanics. The chaotic nature of the de Sitter horizon is assessed through the soft mode action at the AdS 2 boundary, as well as the behaviour of shockwave type solutions.
arXiv:1811.08153v3 [hep-th] 14 Jul 2019Several thermodynamic features of the de Sitter horizon have been known since the classic work of Gibbons and Hawking [1]. What is missing so far, is a framework to bridge the gap between the thermodynamic and microscopic, in the same spirit that AdS/CFT bridges the gap between the old literature on black hole thermodynamics and the modern perspective of a holographic liquid.What makes the de Sitter problem challenging is the absence of a spatial AdS boundary, or more generally some non-gravitating region of spacetime, from which to probe the de Sitter horizon. To address this, we construct a phenomenological gravitational theory which contains asymptotically AdS solutions with a region of de Sitter in the deep interior. Our approach is inspired, to an extent, by analogous approaches applying the framework of AdS/CFT to problems in condensed matter [2]. Though this approach is incomplete, we believe that bringing the question of the de Sitter horizon to the standards of AdS/CMT is a step in the forward direction. Ultimately, a successful approach will require a microscopic completion.Concretely, we construct a class of two-dimensional gravitational theories admitting solutions which interpolate between an AdS 2 boundary with a dS 2 horizon in the deep interior [3]. Having done so, we probe the de Sitter horizon using the available tools of AdS/CFT. There are several reasons to work in two-dimensions. Though simpler, the dS 2 horizon shares many features with its higher dimensional cousin, including the characteristics of its quasinormal modes [4] and the finiteness of the geometry. Also, dS 2 × S 2 appears as solution of Einstein gravity with Λ > 0 [5] and hence dS 2 is directly relevant to four-dimensional de Sitter. Furthermore, recent progress in our microscopic understanding of AdS 2 holography [6,7,8,9,10,11,12,13] may guide us in constructing a microscopic model dual to the interpolating geometry.Embedding an inflating universe in an AdS d+1 spacetime with d > 1 was previously considered in the interesting works of [14,15]. There, essentially due to the Raychadhuri equation combined with the null energy condition, it was found the de Sitter region lived within the Schwarzschild-AdS black hole horizon. It would seem, then, that discovering the de Sitter horizon is at least as complicated as solving the notorious puzzle of the region interior to the horizon.The two-dimensional geometries we consider have the ad...