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Non-extremal fuzzballs and ergoregion emission

Borun D. Chowdhury, Samir D. Mathur

Abstract

In the traditional picture of black holes Hawking radiation is created by pair creation from the vacuum at the horizon. In the fuzzball proposal, individual microstates do not have a horizon with the `vacuum' state in its vicinity. For a special family of non-extremal microstates it was recently found that emission occurs due to pair creation in an ergoregion, rather than at a horizon. In this paper we extend this result to a slightly larger class of microstates, again finding exact agreement between the emission in the gravity picture and the CFT dual. We write down an expression for emission from geometries with ergoregions, in terms of the leading falloff behavior of the wavefunctions in the fuzzball region. Finally, we describe another family of nonextremal microstates and find their ergoregion.

Non-extremal fuzzballs and ergoregion emission

Abstract

In the traditional picture of black holes Hawking radiation is created by pair creation from the vacuum at the horizon. In the fuzzball proposal, individual microstates do not have a horizon with the `vacuum' state in its vicinity. For a special family of non-extremal microstates it was recently found that emission occurs due to pair creation in an ergoregion, rather than at a horizon. In this paper we extend this result to a slightly larger class of microstates, again finding exact agreement between the emission in the gravity picture and the CFT dual. We write down an expression for emission from geometries with ergoregions, in terms of the leading falloff behavior of the wavefunctions in the fuzzball region. Finally, we describe another family of nonextremal microstates and find their ergoregion.

Paper Structure

This paper contains 36 sections, 121 equations, 6 figures.

Figures (6)

  • Figure 1: The NS vacuum is shown in (a) and the chiral primary state is shown in (b).
  • Figure 2: The ground state in the twisted Ramond sector.
  • Figure 3: The initial state of the CFT; each component string has a certain winding number and left and right fermionic excitations.
  • Figure 4: The state of the CFT after one 'final state' component string has been produced.
  • Figure 5: A generic stationary geometry (in the large $R$ limit).
  • ...and 1 more figures