12
views
0
recommends
+1 Recommend
0 collections
    0
    shares
      • Record: found
      • Abstract: found
      • Article: found
      Is Open Access

      Fluctuating Black Hole Horizons

      Preprint

      Read this article at

      Bookmark
          There is no author summary for this article yet. Authors can add summaries to their articles on ScienceOpen to make them more accessible to a non-specialist audience.

          Abstract

          In this paper we treat the black hole horizon as a physical boundary to the spacetime and study its dynamics following from the Gibbons-Hawking-York boundary term. Using the Kerr black hole as an example we derive an effective action that describes, in the large wave number limit, a massless Klein-Gordon field living on the average location of the boundary. Complete solutions can be found in the small rotation limit of the black hole. The formulation suggests that the boundary can be treated in the same way as any other matter contributions. In particular, the angular momentum of the boundary matches exactly with that of the black hole, suggesting an interesting possibility that all charges (including the entropy) of the black hole are carried by the boundary. Using this as input, we derive predictions on the Planck scale properties of the boundary.

          Related collections

          Most cited references12

          • Record: found
          • Abstract: found
          • Article: found
          Is Open Access

          Shear viscosity of strongly coupled N=4 supersymmetric Yang-Mills plasma

          , , (2010)
          Using the anti-de Sitter/conformal field theory correspondence, we relate the shear viscosity \eta of the finite-temperature N=4 supersymmetric Yang-Mills theory in the large N, strong-coupling regime with the absorption cross section of low-energy gravitons by a near-extremal black three-brane. We show that in the limit of zero frequency this cross section coincides with the area of the horizon. From this result we find \eta=\pi/8 N^2T^3. We conjecture that for finite 't Hooft coupling (g_YM)^2N the shear viscosity is \eta=f((g_YM)^2N) N^2T^3, where f(x) is a monotonic function that decreases from O(x^{-2}\ln^{-1}(1/x)) at small x to \pi/8 when x\to\infty.
            Bookmark
            • Record: found
            • Abstract: found
            • Article: found
            Is Open Access

            Quasilocal Energy and Conserved Charges Derived from the Gravitational Action

            The quasilocal energy of gravitational and matter fields in a spatially bounded region is obtained by employing a Hamilton-Jacobi analysis of the action functional. First, a surface stress-energy-momentum tensor is defined by the functional derivative of the action with respect to the three-metric on \({}^3B\), the history of the system's boundary. Energy density, momentum density, and spatial stress are defined by projecting the surface stress tensor normally and tangentially to a family of spacelike two-surfaces that foliate \({}^3B\). The integral of the energy density over such a two-surface \(B\) is the quasilocal energy associated with a spacelike three-surface \(\Sigma\) whose intersection with \({}^3B\) is the boundary \(B\). The resulting expression for quasilocal energy is given in terms of the total mean curvature of the spatial boundary \(B\) as a surface embedded in \(\Sigma\). The quasilocal energy is also the value of the Hamiltonian that generates unit magnitude proper time translations on \({}^3B\) in the direction orthogonal to \(B\). Conserved charges such as angular momentum are defined using the surface stress tensor and Killing vector fields on \({}^3B\). For spacetimes that are asymptotically flat in spacelike directions, the quasilocal energy and angular momentum defined here agree with the results of Arnowitt-Deser-Misner in the limit that the boundary tends to spatial infinity. For spherically symmetric spacetimes, it is shown that the quasilocal energy has the correct Newtonian limit, and includes a negative contribution due to gravitational binding.
              Bookmark
              • Record: found
              • Abstract: found
              • Article: found
              Is Open Access

              The holographic principle

              There is strong evidence that the area of any surface limits the information content of adjacent spacetime regions, at 10^(69) bits per square meter. We review the developments that have led to the recognition of this entropy bound, placing special emphasis on the quantum properties of black holes. The construction of light-sheets, which associate relevant spacetime regions to any given surface, is discussed in detail. We explain how the bound is tested and demonstrate its validity in a wide range of examples. A universal relation between geometry and information is thus uncovered. It has yet to be explained. The holographic principle asserts that its origin must lie in the number of fundamental degrees of freedom involved in a unified description of spacetime and matter. It must be manifest in an underlying quantum theory of gravity. We survey some successes and challenges in implementing the holographic principle.
                Bookmark

                Author and article information

                Journal
                20 May 2013
                2013-10-07
                Article
                10.1007/JHEP10(2013)195
                1305.4461
                a4038096-d0b7-4de9-9611-741f88b66895

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                References added, nature of boundary stress tensor clarified, discussion of statistics refined and a mistake with Hawking temperature corrected, 16 pages; version to appear in journal
                gr-qc hep-th

                Comments

                Comment on this article