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Orbits and Attractors for N=2 Maxwell-Einstein Supergravity Theories in Five Dimensions

High Energy Physics - Theory · Submitted 12 Jun 2006

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Motivated by these results and some recent work on non-supersymmetric attractors we show that attractor equations in N=2 MESGTs in d=5 do indeed possess the distinct families of solutions with finite Bekenstein-Hawking entropy.

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arXiv IDhep-th/0606108 (version 2)
Pith ID2KOD33O5, Pith's permanent record of this paper and its review
CitationMurat Gunaydin, Sergio Ferrara. "Orbits and Attractors for N=2 Maxwell-Einstein Supergravity Theories in Five Dimensions." arXiv:hep-th/0606108 (2006). https://pith.science/paper/2KOD33O5
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What the abstract itself states, as probabilities: claims first 0.07 · states limitation 0.53 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.09 · compares with prior results 0.85 · mentions code or data availability 0.01.

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arXiv listing abstract v2. Results and the main claim are underlined; .

BPS and non-BPS orbits for extremal black-holes in N=2 Maxwell-Einstein supergravity theories (MESGT) in five dimensions were classified long ago by the present authors for the case of symmetric scalar manifolds. Motivated by these results and some recent work on non-supersymmetric attractors we show that attractor equations in N=2 MESGTs in d=5 do indeed possess the distinct families of solutions with finite Bekenstein-Hawking entropy. The new non-BPS solutions have non-vanishing central charge and matter charge which is invariant under the maximal compact subgroup of the stabilizer of the non-BPS orbit. Our analysis covers all symmetric space theories G/H such that G is a symmetry of the action. These theories are in one-to-one correspondence with (Euclidean) Jordan algebras of degree three. In the particular case of N=2 MESGT with scalar manifold SU*(6)/USp(6) a duality of the two solutions with regard to N=2 and N=6 supergravity is also considered.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 BPS and non-BPS orbits for extremal black-holes in N=2 Maxwell-Einstein supergravity theories (MESGT) in five dimensions were classified long ago by the present authors for the case of symmetric scalar manifolds. background 1.00 0.78 0.04 asserted 1.00
s1 Motivated by these results and some recent work on non-supersymmetric attractors we show that attractor equations in N=2 MESGTs in d=5 do indeed possess the distinct families of solutions with finite Bekenstein-Hawking entropy. result 0.64 0.91 0.78 asserted 1.00
s2 The new non-BPS solutions have non-vanishing central charge and matter charge which is invariant under the maximal compact subgroup of the stabilizer of the non-BPS orbit. result 1.00 0.86 0.21 asserted 1.00
s3 Our analysis covers all symmetric space theories G/H such that G is a symmetry of the action. contribution 0.79 0.71 0.07 asserted 1.00
s4 These theories are in one-to-one correspondence with (Euclidean) Jordan algebras of degree three. background 0.80 0.22 0.04 asserted 1.00
s5 In the particular case of N=2 MESGT with scalar manifold SU*(6)/USp(6) a duality of the two solutions with regard to N=2 and N=6 supergravity is also considered. contribution 0.68 0.81 0.05 asserted 0.90

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Original abstract

BPS and non-BPS orbits for extremal black-holes in N=2 Maxwell-Einstein supergravity theories (MESGT) in five dimensions were classified long ago by the present authors for the case of symmetric scalar manifolds. Motivated by these results and some recent work on non-supersymmetric attractors we show that attractor equations in N=2 MESGTs in d=5 do indeed possess the distinct families of solutions with finite Bekenstein-Hawking entropy. The new non-BPS solutions have non-vanishing central charge and matter charge which is invariant under the maximal compact subgroup of the stabilizer of the non-BPS orbit. Our analysis covers all symmetric space theories G/H such that G is a symmetry of the action. These theories are in one-to-one correspondence with (Euclidean) Jordan algebras of degree three. In the particular case of N=2 MESGT with scalar manifold SU*(6)/USp(6) a duality of the two solutions with regard to N=2 and N=6 supergravity is also considered.

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23 arXiv papers cite this in 33 sentences

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  • We can compare the eigenvalues of the 3x3 part of the fermion mass matrix with the eigenvalues of the 3x3 octonionic Hermitian matrix studied in [ref] which defines the supersymmetric black hole entropy in 5d.

    M-theory, Black Holes and Cosmology · Properties of the mass matrix in octonion cosmological models · 0.99

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