20–24 Jul 2015
Frankfurt Institute for Advanced Studies
Europe/Berlin timezone

Session

Student plenary session 1

students1
20 Jul 2015, 14:00
Frankfurt Institute for Advanced Studies

Frankfurt Institute for Advanced Studies

Goethe-Universität FrankfurtCampus Riedberg Ruth-Moufang-Straße 1 60438 Frankfurt am Main GERMANY

Description

15+5 min talks.
Chair: Dennis D. Dietrich

Presentation materials

There are no materials yet.

  1. Ali Seraj (IPM, Tehran, Iran)
    20/07/2015, 14:00
    Students
    We construct the classical phase space of Near-Horizon Extremal Geometries with fixed angular momenta and entropy. Each element in the phase space is a geometry with SL(2,R)×U(1)d−3 Killing isometries which has vanishing SL(2,R) and constant U(1) charges. In four spacetime dimensions, the symmetry algebra consists of the familiar Virasoro algebra, while in d>4 dimensions the symmetry algebra,...
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  2. Mr Mattia Colombo (University of Nottingham)
    20/07/2015, 14:20
    Students
    When Lorentz symmetry is broken, defining the concept of Black Hole becomes highly non-trivial. In this talk I wish to discuss the problems related to such definition and introduce a way to define the causal structure and horizons for a manifold with a preferred foliation.
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  3. Ms Marcela Cárdenas (Universidad de Concepción, Centro de Estudios Científicos)
    20/07/2015, 14:40
    Students
    We present a Chern-Simons-like description of three-dimensional gravity with negative cosmological constant, where the matter source is a conformally coupled real scalar field. This description is based on a first-order action that provides a set of field equations equivalent to that derived from the usual second-order action. The system admits a rotating hairy black hole solution, which is...
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  4. Andrea Giugno (University of Bologna)
    20/07/2015, 15:00
    Students
    We study a corpuscular model of evaporating black holes consisting of a large number $N$ of self-confined bosons. The single-particle spectrum contains a discrete ground state of energy $m$ (corresponding to toy gravitons forming a black hole), and a gapless continuous spectrum (to accommodate for Hawking radiation with energy $\omega>m$). In particular, we consider each constituent in a...
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