Abstract

We perform Hamiltonian reduction of a model in which 2 + 1 dimensional gravity with negative cosmological constant is coupled to a cylindrically symmetric dust shell. The resulting action contains only a finite number of degrees of freedom. The phase space consists of two copies of ADS2—both coordinate and momentum space are curved. Different regions in the Penrose diagram can be identified with different patches of ADS2 momentum space. Quantization in the momentum representation becomes particularly simple in the vicinity of the horizon, where one can neglect momentum non-commutativity. In this region, we calculate the spectrum of the shell radius. This spectrum turns out to be continuous outside the horizon and becomes discrete inside the horizon with eigenvalue spacing proportional to the square root of the black hole mass. We also calculate numerically quantum transition amplitudes between different regions of the Penrose diagram in the vicinity of the horizon. This calculation shows a possibility of quantum tunneling of the shell into classically forbidden regions of the Penrose diagram, although with an exponentially damped rate away from the horizon.

Highlights

  • General Relativity encounters problems at short distances both at a classical and quantum level.Classical gravity develops singularities, while there are ultraviolet divergences in quantum gravity which cannot be removed by renormalization.On the other hand, as it was first argued by Bronstein [1], there is the smallest possible distance in quantum gravity, the Planck length, beyond which measurements are not possible

  • We calculate numerically quantum transition amplitudes between different regions of the Penrose diagram in the vicinity of the horizon. This calculation shows a possibility of quantum tunneling of the shell into classically forbidden regions of the Penrose diagram, with an exponentially damped rate away from the horizon

  • We focus on studying quantum dynamics in the near-horizon area, where quantization could be performed by traditional methods due to momentum commutativity

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Summary

Introduction

General Relativity encounters problems at short distances both at a classical and quantum level. The only difference between this result in 2 + 1 and 3 + 1 dimensional gravity is the absence of Newtonian potential and a contribution from cosmological constant, but the solution to the constraints branches in the same way. This constraint turns out to be slightly different from that of [14,15]. We will look for a real chart that would cover the entire phase space of the model

Global Parameterization of ADS and BTZ Spacetime
Action Principle and Symplectic Form
Constraints
Derivation of the Constraint Equations
Quantization
Quantum Dynamics
Conclusions
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