Gauged N = 8 d = 5 supergravity

Pernici, M.; Pilch, Krzysztof; Nieuwenhuizen, P. van

doi:10.1016/0550-3213(85)90645-5

Cited by 183 publications

(287 citation statements)

References 19 publications

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“…Although N = 8 was formulated back in 80's [1][2][3], very few analytic solutions have been constructed explicitely in this theory [4], since most of them are also solutions to the less supersymmetric truncations, which are more straightforward to approach [5][6][7][8][9][10][11][12][13][14][15][16][17][18][19].…”

Section: Jhep03(2014)057mentioning

confidence: 99%

“…Therefore, even if distinct, all such spacetimes deserve the name black branes. 2 The distinction between black strings and black rings is a notable exception of the general rule, as it arises from the global embedding of the near-horizon geometry in the full spacetime (black rings are also special in the fact that they exist only in flat space) [30]. One can then say that black strings have AdS3 factors near their horizon, while for black rings the AdS is substituted by an extremal BTZ black hole.…”

Section: Jhep03(2014)057mentioning

confidence: 99%

“…In particular in the following sections we will be interested in vacua that break the gauge symmetry to SO(3)×SO(3) or SO(4)×SO (2). Notice that both these groups contain nonabelian factors, and thus allow for the possibility to explore solutions with gravity coupled to nonabelian gauge fields, which is of main interest here.…”

Section: Jhep03(2014)057mentioning

confidence: 99%

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Attractors, black objects and holographic RG flows in 5d maximal gauged supergravities

Hristov

Rota

2014

J. High Energ. Phys.

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We perform a systematic search for static solutions in different sectors of 5d N = 8 supergravities with compact and non-compact gauged R-symmetry groups, finding new and listing already known backgrounds. Due to the variety of possible gauge groups and resulting scalar potentials, the maximally symmetric vacua we encounter in these theories can be Minkowski, de Sitter, or anti-de Sitter. There exist BPS and non-BPS near-horizon geometries and full solutions with all these three types of asymptotics, corresponding to black holes, branes, strings, rings, and other black objects with more exotic horizon topologies, supported by U(1) and SU(2) charges. The asymptotically AdS 5 solutions also have a clear holographic interpretation as RG flows of field theories on D3 branes, wrapped on compact 2-and 3-manifolds.

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Section: Jhep03(2014)057mentioning

confidence: 99%

Section: Jhep03(2014)057mentioning

confidence: 99%

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Attractors, black objects and holographic RG flows in 5d maximal gauged supergravities

Hristov

Rota

2014

J. High Energ. Phys.

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“…In particular the flows of N = 4 supersymmetric Yang-Mills theories under "bilinear perturbations 1 " has been extensively studied [1][2][3][4][5][6][7][8][9][10][11] using gauged N = 8 supergravity in five dimensions [12,13]. The most extensive studies have been made for supersymmetric flows because these are generically simpler, more controllable, and sometimes enable direct comparisons of the supergravity and field theory limits.…”

Section: Introductionmentioning

confidence: 99%

A class of supersymmetric RG flows from five-dimensional supergravity

Khavaev

Warner

2000

Physics Letters B

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We consider the holographic dual of a general class of N = 1 * flows in which all three chiral multiplets have independent masses, and in which the corresponding Yang-Mills scalars can develop particular supersymmetry-preserving vevs. We also allow the gaugino to develop a vev. This leads to a six parameter subspace of the supergravity scalar action, and we show that this is a consistent truncation, and obtain a superpotential that governs the N = 1 * flows on this subspace. We analyse some of the structure of the superpotential, and check consistency with the asymptotic behaviour near the UV fixed point. We show that the dimensions of the six couplings obey a sum rule all along the N = 1 * flows. We also show how our superpotential describes part of the Coulomb branch of the non-trivial N = 1 fixed point theory.

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“…the four-form C 4 has a self-dual field strengthF 5 . Type IIB supergravity is constructed through supersymmetry and gauge arguments [76,77] starting from the equations of motion. Further it was shown that supergravity is stable on anti de Sitter spaces [78, for supergravity in 5 dimensions] with an appropriate set of boundary conditions.…”

Section: Supergravity and Anti-de Sitter Spacementioning

confidence: 99%

Holographic quark gluon plasma with flavor

Kaminski

2009

Fortschritte der Physik

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In this work I explore theoretical and phenomenological implications of chemical potentials and charge densities inside a strongly coupled thermal plasma, using the gauge/gravity correspondence. Strong coupling effects discovered in this model theory are interpreted geometrically and may be taken as qualitative predictions for heavy ion collisions at RHIC and LHC. In particular I examine the thermodynamics, spectral functions, transport coefficients and the phase diagram of the strongly coupled plasma. For example stable mesons, which are the analogs of the QCD Rho-mesons, are found to survive beyond the deconfinement transition. This paper is based on partly unpublished work performed in the context of my PhD thesis. New results and ideas extending significantly beyond those published until now are stressed.

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Gauged N = 8 d = 5 supergravity

Cited by 183 publications

References 19 publications

Attractors, black objects and holographic RG flows in 5d maximal gauged supergravities

Attractors, black objects and holographic RG flows in 5d maximal gauged supergravities

A class of supersymmetric RG flows from five-dimensional supergravity

Holographic quark gluon plasma with flavor

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