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Related papers: D=5 M-theory radion supermultiplet dynamics

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It has been known that D=5 simple supergravity resembles D=11 supergravity in many respects. We present their further resemblances in (1) the duality groups upon dimensional reduction, and (2) the worldsheet structure of the solitonic…

High Energy Physics - Theory · Physics 2009-10-31 S. Mizoguchi , N. Ohta

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

Four dimensional supergravities may be the right framework to describe particle physics at low energies. Its connection to the underlying string theory can be implemented through higher dimensional supergravities which bear special…

High Energy Physics - Theory · Physics 2014-04-23 G. A. Diamandis , B. C. Georgalas , P. Kouroumalou , A. B. Lahanas

A supersymmetric non-Abelian self-dual gauge theory with the explicit introduction of Kaluza-Klein modes is proposed to give a classical description of multiple M5-branes on $R^5 \times S^1$. The gauge symmetry is parametrized by…

High Energy Physics - Theory · Physics 2015-06-22 Pei-Ming Ho , Yutaka Matsuo

We study the properties of branes in supergravity theory. We investigate a class of systems consisting of an M5-brane in the Kaluza-Klein monopole background with 1/4 supersymmetry in 11-dimensions. In the near core region of the…

High Energy Physics - Theory · Physics 2007-05-23 Masako Asano

We derive superalgebras in many types of supersymmetric M-brane backgrounds. The backgrounds examined here include the cases of the M-wave and the M-Kaluza-Klein monopole. On the basis of the obtained algebras, we deduce all the…

High Energy Physics - Theory · Physics 2009-10-31 Takeshi Sato

We compute the two-derivative low-energy effective action for the radion in the (supersymmetric) Randall-Sundrum scenario with detuned brane tensions. At the classical level, a potential automatically stabilizes the distance between the…

High Energy Physics - Theory · Physics 2009-11-10 Jonathan Bagger , Michele Redi

The (4,0) supermultiplet in 6 dimensions contains a 4th rank tensor gauge field with the symmetries of the Riemann tensor and is superconformal, with 32+32 supersymmetries. Dimensional reduction on a circle gives the 5D N=8 supergravity…

High Energy Physics - Theory · Physics 2022-09-26 Chris Hull

We supersymmetrize a class of moduli dependent potentials living on branes with the help of additional bulk terms in 5d N=2 supergravity. The space of Poincare invariant vacuum solutions includes the Randall-Sundrum solution and the…

High Energy Physics - Theory · Physics 2009-10-31 Adam Falkowski , Zygmunt Lalak , Stefan Pokorski

We compute the one-loop correction to the radion potential in the Randall-Sundrum model with detuned brane tensions, with supersymmetry broken by boundary conditions. We concentrate on the small-warping limit, where the one-loop correction…

High Energy Physics - Theory · Physics 2008-11-26 Andrey Katz , Yael Shadmi , Yuri Shirman

We present the explicit form of the four-dimensional effective supergravity action which describes low-energy physics of the Randall--Sundrum model with moduli fields in the bulk and charged chiral matter living on the branes. The…

High Energy Physics - Theory · Physics 2009-11-07 Zygmunt Lalak

In this brief report, we summarize our recent studies in brane cosmology in both string theory and M-Theory on $S^{1}/Z_{2}$. In such setups, we find that the radion is stable and its mass, with a very conservative estimation, can be of the…

High Energy Physics - Phenomenology · Physics 2010-03-29 Anzhong Wang

Solitonic brane cosmologies are found where the world-volume is curved due to the evolution of the dilaton field on the brane. In many cases, these may be related to the solitonic Dp- and M5-branes of string and M-theory. An…

High Energy Physics - Theory · Physics 2009-10-31 James E. Lidsey

We study wrapped brane configurations via possible maximally supersymmetric gauged supergravities. First, we construct various supersymmetric wrapped D3 brane configurations from D=5 N=8 SO(6) gauged supergravity. This procedure provides…

High Energy Physics - Theory · Physics 2007-05-23 Michihiro Naka

We give a formulation of linearized minimal 5-dimensional supergravity in N = 1 superspace. Infinitesimal local 5D diffeomorphisms, local 5D Lorentz transformations, and local 5D supersymmetry are all realized as off-shell superfield…

High Energy Physics - Theory · Physics 2008-11-26 W. D. Linch , Markus A. Luty , J. Phillips

We examine the moduli dynamics of a specific class of supergravity-inspired BPS braneworlds, clarifying the role of bulk scalar fields in brane collisions. The model contains as a special case the Randall-Sundrum model both with and without…

High Energy Physics - Theory · Physics 2007-05-23 S. L. Webster , A. C. Davis

We examine Kaluza-Klein branes in detail. Specifically, we show that codimension four submanifolds that are stationary under a semi-free circle action may be interpreted as branes or antibranes in the Kaluza-Klein reduced space that are…

High Energy Physics - Theory · Physics 2007-05-23 J. F. Sparks

We explicitly construct a solution of eight-dimensional gauged supergravity representing D6-branes wrapped on six-cycles inside Calabi-Yau fourfolds. The solution preserves two supercharges and asymptotically is a cone with the coset space…

High Energy Physics - Theory · Physics 2010-04-05 Rafael Hernandez , Konstadinos Sfetsos

We look at the vertical dimensional reduction of the supermembrane of M-theory to the D2-brane of Type IIA string theory. Our approach considers the soliton solutions of the two low energy field limits, D=11 and D=10 Type IIA…

High Energy Physics - Theory · Physics 2009-10-31 C. Codirla , M. J. Perry

The near-horizon geometry of parallel NS5-branes is described by an exact superconformal 2d field theory based on K^10 = W(k)^4 x M^6, with M^6 a flat 5+1 space time and W(k)^4 =U(1) x SU(2)(k), a four dimensional background with…

High Energy Physics - Theory · Physics 2015-06-25 Costas Kounnas