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Black Holes and U-Duality

Mirjam Cvetic, Christopher M. Hull

TL;DR

This work constructs the most general charged rotating black holes in $4\le D\le 9$ from toroidally compactified Type II/String/M-theory by starting from a minimal generating solution and acting with the classical duality group, thereby generating all charge configurations without changing the Einstein-frame metric. It shows that the full set of solutions can be obtained via orbits of the maximal compact subgroups ($C_U$) of the duality groups, yielding explicit charge counting commensurate with the dimension of the charge lattice. For BPS-saturated static black holes, the horizon area and ADM mass can be expressed in duality-invariant forms: in $D=4$ via the quartic invariant $J_4$ of $E_{7(7)}$, in $D=5$ via the cubic invariant $J_3$ of $E_{6(6)}$, while in $D\ge 6$ such invariants vanish and the horizon area is zero. The results illuminate how microscopic entropy should depend only on duality-invariant combinations of bare charges, and they provide a procedure to obtain manifestly $U$-duality invariant mass formulas across dimensions, with explicit connections to known attractor-type behavior for BPS black holes.

Abstract

We find the general charged rotating black hole solutions of the maximal supergravities in dimensions $4\le D\le 9$ arising from toroidally compactified Type II string or M-theories. In each dimension, these are obtained by acting on a generating solution with classical duality symmetries. In D=4, D=5 and $6\le D \le 9$ the generating solution is specified by the ADM mass, $[{D-1}/2]$-angular momentum components and five, three and two charges, respectively. We discuss the BPS-saturated (static) black holes and derive the U-duality invariant form of the area of the horizon. We also comment on the U-duality invariant form of the BPS mass formulae.

Black Holes and U-Duality

TL;DR

This work constructs the most general charged rotating black holes in from toroidally compactified Type II/String/M-theory by starting from a minimal generating solution and acting with the classical duality group, thereby generating all charge configurations without changing the Einstein-frame metric. It shows that the full set of solutions can be obtained via orbits of the maximal compact subgroups () of the duality groups, yielding explicit charge counting commensurate with the dimension of the charge lattice. For BPS-saturated static black holes, the horizon area and ADM mass can be expressed in duality-invariant forms: in via the quartic invariant of , in via the cubic invariant of , while in such invariants vanish and the horizon area is zero. The results illuminate how microscopic entropy should depend only on duality-invariant combinations of bare charges, and they provide a procedure to obtain manifestly -duality invariant mass formulas across dimensions, with explicit connections to known attractor-type behavior for BPS black holes.

Abstract

We find the general charged rotating black hole solutions of the maximal supergravities in dimensions arising from toroidally compactified Type II string or M-theories. In each dimension, these are obtained by acting on a generating solution with classical duality symmetries. In D=4, D=5 and the generating solution is specified by the ADM mass, -angular momentum components and five, three and two charges, respectively. We discuss the BPS-saturated (static) black holes and derive the U-duality invariant form of the area of the horizon. We also comment on the U-duality invariant form of the BPS mass formulae.

Paper Structure

This paper contains 33 sections, 64 equations, 1 table.