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Related papers: Intersecting M-branes as Four-Dimensional Black Ho…

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We present non-extreme generalisations of intersecting p-brane solutions of eleven-dimensional supergravity which upon toroidal compactification reduce to non-extreme static black holes in dimensions D=4, D=5 and 5<D<10, parameterized by…

High Energy Physics - Theory · Physics 2009-09-17 M. Cvetic , A. A. Tseytlin

We present new supersymmetric solutions of D=11 supergravity obtained by intersecting the brane configuration interpreted as a 2-brane lying within a 5-brane. Some of these solutions can be boosted along a common string and/or superposed…

High Energy Physics - Theory · Physics 2009-10-30 Miguel S. Costa

We present intersecting p-brane solutions of eleven-dimensional supergravity (M-branes) which upon toroidal compactification reduce to non-extreme ``rotating'' black holes. We identify harmonic functions, associated with each M-brane, and…

High Energy Physics - Theory · Physics 2009-09-17 Mirjam Cvetic , Donam Youm

We present solutions describing supersymmetric configurations of 2 or 3 orthogonally intersecting 2-branes and 5-branes of D=11 supergravity. The configurations which preserve 1/4 or 1/8 of maximal supersymmetry are 2+2, 5+5, 2+5, 2+2+2,…

High Energy Physics - Theory · Physics 2009-09-17 A. A. Tseytlin

An M-brane and anti-M-brane scheme is proposed to study nonextremal 4D and 5D black holes. The improved nonextremal intersecting M-brane solutions proposed here, involve two sets of harmonic functions. The constraints among the pressures…

High Energy Physics - Theory · Physics 2009-10-30 Jian-Ge Zhou , H. J. W. Mueller-Kirsten , J. -Q. Liang , F. Zimmerschied

We find extremal four dimensional black holes with finite area constructed entirely from intersecting D-branes. We argue that the microscopic degeneracy of these configurations agrees with the Bekenstein-Hawking entropy formula. The absence…

High Energy Physics - Theory · Physics 2011-05-05 Vijay Balasubramanian , Finn Larsen

We construct the most general supersymmetric configuration of D2-branes and D6-branes on a 6-torus. It contains arbitrary numbers of branes at relative U(3) angles. The corresponding supergravity solutions are constructed and expressed in a…

High Energy Physics - Theory · Physics 2016-08-25 V. Balasubramanian , F. Larsen , R. G. Leigh

We discuss special supersymmetric extreme black holes in 4 and 5 dimensions which have regular horizons, non-zero entropy and can be interpreted as compactifications of BPS bound states of p-branes in 10 or 11 dimensions.

General Relativity and Quantum Cosmology · Physics 2007-05-23 A. A. Tseytlin

We start with BPS-saturated configurations of two (orthogonally) intersecting M-branes and use the electro-magnetic duality or dimensional reduction along a boost, in order to obtain new p-brane bound states. In the first case the resulting…

High Energy Physics - Theory · Physics 2009-09-17 Miguel S. Costa , Mirjam Cvetic

In this paper we construct the BPS black hole generating solution of toroidally compactified string (and M) theory, giving for it both the macroscopic and microscopic description. Choosing a proper U-duality gauge the latter will be given…

High Energy Physics - Theory · Physics 2010-11-19 M. Bertolini , M. Trigiante

The supersymmetric p-branes of Type II string theory can be interpreted after compactification as extremal black holes with zero entropy and infinite temperature. We show how the p-branes avoid this apparent, catastrophic instability by…

High Energy Physics - Theory · Physics 2009-10-30 Vijay Balasubramanian , Finn Larsen

We propose a formulation of 11-dimensional M-theory in terms of five-branes with closed strings on their world-volume. We use this description to construct the complete spectrum of BPS states in compactifications to six and five dimensions.…

High Energy Physics - Theory · Physics 2009-07-09 R. Dijkgraaf , E. Verlinde , H. Verlinde

We construct new configurations of oppositely charged, static black hole pairs (diholes) in four dimensions which are solutions of low energy string/M-theory. The black holes are extremal and have four different charges. We also consider…

High Energy Physics - Theory · Physics 2010-04-28 Auttakit Chattaraputi , Roberto Emparan , Anne Taormina

We explore the connection between D-branes and black holes in one particular case: a $D3$-brane compactified to four dimensions on $T^6/Z_3$. Using the $D$-brane boundary state description we show the equivalence with a double extremal N=2…

High Energy Physics - Theory · Physics 2009-03-27 M. Bertolini , P. Fre , F. Hussain , R. Iengo , C. Nunez , C. Scrucca

We present the magnetic duals of G\"uven's electric-type solutions of D=11 supergravity preserving $1/4$ or $1/8$ of the D=11 supersymmetry. We interpret the electric solutions as $n$ orthogonal intersecting membranes and the magnetic…

High Energy Physics - Theory · Physics 2009-10-09 G. Papadopoulos , P. K. Townsend

We investigate the possibility of extending non-extreme black hole solutions made of intersecting M-branes to those with two non-extreme deformation parameters, similar to Reissner-Nordstr{\o}m solutions. General analysis of possible…

High Energy Physics - Theory · Physics 2008-12-18 Nobuyoshi Ohta , Takashi Shimizu

We study intersecting D-branes in type 0 string theories and show that the D$p_{\pm}$-brane bound states obey similar intersecting rules as the D$p$-branes of the type II theories. The D$5_{\pm}$-D$1_{\pm}$ brane system is studied in…

High Energy Physics - Theory · Physics 2010-12-03 Miguel S. Costa

We construct new supersymmetric solutions of $D$=11 supergravity describing $n$ orthogonally ``overlapping" membranes and fivebranes for $n$=2,\dots,8. Overlapping branes arise after separating intersecting branes in a direction transverse…

High Energy Physics - Theory · Physics 2009-10-30 Jerome P. Gauntlett , David A. Kastor , Jennie Traschen

We establish the relation between the structure governing supersymmetric and non-supersymmetric four- and five-dimensional black holes and multicenter solutions and Calabi-Yau flux compactifications of M-theory and type IIB string theory.…

High Energy Physics - Theory · Physics 2015-06-05 Iosif Bena , Hagen Triendl , Bert Vercnocke

We discuss the known microscopic interpretations of the Bekenstein-Hawking entropy for configurations of intersecting M-branes. In some cases the entropy scales as that of a massless field theory on the intersection. A different situation,…

High Energy Physics - Theory · Physics 2009-09-17 I. R. Klebanov , A. A. Tseytlin
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