Artikel,

Einstein Gravity as a Conformal Field Theory on Horizons of Stationary and Axisymmetric Black Holes

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(18.08.2011)

Zusammenfassung

We carry out a Kaluza-Klein reduction of the Einstein-Hilbert action along the ignorable coordinates of stationary and axisymmetric black holes. Rigid diffeomorphism invariance of the \$m\$-ignorable coordinates then become a global \$SL(m,R)\$ gauge symmetry of the reduced theory. Mass and angular momentum of the black holes are related to generators of an \$SL(2,R)\$ subgroup of the full symmetry. Related to each angular momentum there is also an \$SL(2,R)\$ subgroup. On the horizon, this \$SL(2,R)\$ can be extended to the full Witt algebra, which is an exact symmetry of the reduced action when the black hole temperature is zero. So on the horizon, the Kaluza-Klein reduced action is a conformal field theory. The infinite dimensional symmetries are explicitly broken when the system is at a finite temperature, i.e. when the black hole temperature is nonzero.

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