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Three Charge Supertubes and Black Hole Hair
High Energy Physics - Theory · Submitted 19 Feb 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We study the relation of the tubes to the spinning BMPV black hole, and find that they have properties consistent with describing some of the hair of this black hole.
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The abstract, sentence by sentence
We construct finite size, supersymmetric, tubular D-brane configurations with three charges, two angular momenta and several brane dipole moments. In type IIA string theory these are tubular configurations with D0, D4 and F1 charge, as well as D2, D6 and NS5 dipole moments. These multi-charge generalizations of supertubes might have interesting consequences for the physics of the D1-D5-P black hole. We study the relation of the tubes to the spinning BMPV black hole, and find that they have properties consistent with describing some of the hair of this black hole.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We construct finite size, supersymmetric, tubular D-brane configurations with three charges, two angular momenta and several brane dipole moments. | contribution 1.00 | 0.96 | 0.11 | asserted 1.00 |
| s1 | In type IIA string theory these are tubular configurations with D0, D4 and F1 charge, as well as D2, D6 and NS5 dipole moments. | contribution 0.93 | 0.46 | 0.04 | asserted 1.00 |
| s2 | These multi-charge generalizations of supertubes might have interesting consequences for the physics of the D1-D5-P black hole. | interpretation 0.90 | 0.12 | 0.09 | speculative 0.94 |
| s3 | We study the relation of the tubes to the spinning BMPV black hole, and find that they have properties consistent with describing some of the hair of this black hole. | result 0.83 | 0.96 | 0.81 | hedged possibility 0.67 |
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The paper
Original abstract
We construct finite size, supersymmetric, tubular D-brane configurations with three charges, two angular momenta and several brane dipole moments. In type IIA string theory these are tubular configurations with D0, D4 and F1 charge, as well as D2, D6 and NS5 dipole moments. These multi-charge generalizations of supertubes might have interesting consequences for the physics of the D1-D5-P black hole. We study the relation of the tubes to the spinning BMPV black hole, and find that they have properties consistent with describing some of the hair of this black hole.
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References
How the literature uses it
19 arXiv papers cite this in 45 sentences
Papers citing it · 35 sentences without a confident label
Builds on it 1 paper
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One can generalize the foregoing discussion of mergers to examine a three-charge, two dipole charge supertube [ref] merging with a generic black ring.
Supertubes in Bubbling Backgrounds: Born-Infeld Meets Supergravity · Black rings and three-charge two-dipole-charge supertubes · 0.99
Compares with it 2 papers
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This conclusion is similar to that of [ref] for supertube-black hole mergers.
Supertubes in Bubbling Backgrounds: Born-Infeld Meets Supergravity · Mergers of black rings with two-charge supertubes · 1.00
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This compares to the standard solutions of [ref] , [ref] , [ref] , [ref] , [ref] when expressed in more convenient coordinates - but we will not require that here.
Entropy Functions with 5D Chern-Simons terms · Switching roles of e(0) - p(0) as a form of black ring - black hole interpolation · 0.99
Cites it as support 1 paper
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Obviously, the state-space geometric description will naturally break down at the Planck scale, but the picture is expected to remain rather interesting, and still it is certainly supported by the fact that large bubbles [ref] are needed to resolve singularities persisting in the macroscopic black brane configurations.
Black Strings, Black Rings and State-space Manifold · (v) Physics at the Planck Scale · 0.98
Cites it as background 4 papers
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The $(0,4)$ conformal field theory on the $AdS_3$ boundary describes M5-branes wrapped on 4-cycles in $X_6$ [ref] (the same conformal field theory also describes black rings [ref] .) To define the elliptic genus we introduce potentials for the charges $q^I, q^I$; the R-charge is $q^0$ (for details, see [ref] ).
Quantum Corrections to Bekenstein-Hawking Black Hole Entropy and Gravity Partition Functions · Partition functions from supergravity · 0.85
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Truthfully, Mathur's proposal has motivated a number of interesting studies for the $D_1$-$D_5$ systems and supertubes [ref] .
Black Strings, Black Rings and State-space Manifold · Introduction · 0.80
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Now, it is very well known, in the context of supersymmetric D2-brane supertube solutions in flat spacetime [ref] that the angular momentum induced by the electromagnetic field on the D6-brane can compete with its tension and stabilize it.
Cosmic Topological Defects from Holography · Vortons · 0.82
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