In its formulation as a Chern-Simons theory, three-dimensional general relativity induces a Wess-Zumino-Witten action on spatial boundaries. Treating the horizon of the three-dimensional Euclidean black hole as a boundary, I count the states of the resulting WZW model, and show that they yield the correct Bekenstein-Hawking entropy. The relevant states can be understood as ``would-be gauge'' degrees of freedom that become dynamical at the horizon
The exact formula derived by us earlier for the entropy of a four dimensional nonrotating black hole...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
We derive an exact expression for the partition function of the Euclidean BTZ black hole. Using this...
We derive an exact expression for the partition function of the Euclidean BTZ black hole. Using this...
We derive an exact formula for the dimensionality of the Hilbert space of the boundary states of SU(...
Although we know that black holes are characterized by a temperature and an entropy, we do not yet h...
To explain black hole thermodynamics in quantum gravity, one must introduce constraints to ensure th...
We derive an exact formula for the dimensionality of the Hilbert space of the boundary states of SU(...
The issue of black hole entropy is reexamined within a finite lattice framework along the lines of W...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
We review the black hole entropy calculation in the framework of Loop Quantum Gravity based on the q...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
The exact formula derived by us earlier for the entropy of a four dimensional nonrotating black hole...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
We derive an exact expression for the partition function of the Euclidean BTZ black hole. Using this...
We derive an exact expression for the partition function of the Euclidean BTZ black hole. Using this...
We derive an exact formula for the dimensionality of the Hilbert space of the boundary states of SU(...
Although we know that black holes are characterized by a temperature and an entropy, we do not yet h...
To explain black hole thermodynamics in quantum gravity, one must introduce constraints to ensure th...
We derive an exact formula for the dimensionality of the Hilbert space of the boundary states of SU(...
The issue of black hole entropy is reexamined within a finite lattice framework along the lines of W...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
We review the black hole entropy calculation in the framework of Loop Quantum Gravity based on the q...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
The exact formula derived by us earlier for the entropy of a four dimensional nonrotating black hole...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...
14 pages. 1 figure. Paragraph added on page 7 to clarify the horizon conditionInternational audience...