General matter coupled N=2 , D=5 gauged supergravity
By A. Ceresole, G. Dall’Agata. 2000
250 citations recorded by the source corpus.
We give the full Lagrangean and supersymmetry transformation rules for D=5 , N=2 supergravity interacting with an arbitrary number of vector, tensor and hyper-multiplets, with gauging of the R -symmetry group SU(2)R as well as a subgroup K of the isometries of the scalar manifold. Among the many possible applications, this theory provides the setting where a supersymmetric brane-world scenario could occur. We comment on the presence of AdS vacua and BPS solutions that would be relevant towards a supersymmetric smooth realization of the Randall–Sundrum “alternative to compactification”. We also add some remarks on the connection between this most general 5D fully coupled supergravity model and type IIB theory on the T11 manifold.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/d3f0de349c124d8a64071d8bf932dcc510c00693
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In Astronomy and Astrophysics
- Kostas Skenderis
- R. Kallosh
- A. Proeyen
- Marika Taylor
- G. Dall’Agata
- Andrei Linde
- Ioannis Papadimitriou
- D. Freedman
In Nuclear and High Energy Physics
- R. Kallosh
- Kostas Skenderis
- A. Proeyen
- Marika Taylor
- G. Dall’Agata
- Eric Bergshoeff
- Andrei Linde
- Ioannis Papadimitriou
Citations in the corpus
- Supersymmetry in Singular Spaces (2000, background): “At this point this reproduces the known ’bulk’ actions of 5 dimensions [11, 12, 13, 14].”
- N = 2 supergravity in five dimensions revisited (2004, background): “. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29 C Identities of very special geometry 29 1 1 Introduction Matter-coupled supergravities in five dimensions have attracted renewed attention [1,2] due to the important role they play in the Randall-Sundrum (RS) braneworld scenario [3,4], in ”
- Hypermultiplets, domain walls and supersymmetric attractors (2001, methodology): “ alone, we study the properties and parametrizations of the scalar manifold SU(2,1) SU(2)×U(1) , giving all Killing vectors and prepotentials that allow us to write down 1This requirement appeared in [1] and was then noticed in [11] for BPS instantons and also in [13]. 2 the generic scalar potential”
- Fake supergravity and domain wall stability (2003, background): “ = Wa(φ)τa, where the τa are the three Pauli matrices. In genuine D= 5,N= 2 supergravity, the matrix superpotential is determined by the gaugings of R-symmetry and isometries of the internal geometry [23, 24, 25]. The internal space is the product of a very special manifold (for scalars in vector an”
- Weyl multiplets of N=2 conformal supergravity in five dimensions (2001, background): “With all these developments, it is clear that it is important that there is an independent derivation of the most general matter couplings derived in [ 10 ].”