Search results for "Supergravity"

showing 10 items of 78 documents

On the Super Higgs Effect in Extended Supergravity

2002

We consider the reduction of supersymmetry in N-extended four dimensional supergravity via the super Higgs mechanism in theories without cosmological constant. We provide an analysis largely based on the properties of long and short multiplets of Poincare' supersymmetry. Examples of the super Higgs phenomenon are realized in spontaneously broken N=8 supergravity through the Scherk-Schwarz mechanism and in superstring compactification in presence of brane fluxes. In many models the massive vectors count the difference in number of the translation isometries of the scalar sigma-model geometries in the broken and unbroken phase.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsCompactification (physics)SupergravityHigh Energy Physics::PhenomenologyFOS: Physical sciencesSuperstring theoryFísicaSupersymmetryCosmological constantsymbols.namesakeTheoretical physicsHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)symbolsHiggs bosonBraneHiggs mechanism
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Non-extremal black holes of N = 2, d = 4 supergravity

2011

We propose a generic recipe for deforming extremal black holes into non-extremal black holes and we use it to find and study the non-extremal black-hole solutions of several N=2,d=4 supergravity models (SL(2,R)/U(1), CPn and STU with four charges). In all the cases considered, the non-extremal family of solutions smoothly interpolates between all the different extremal limits, supersymmetric and not supersymmetric. This fact can be used to find explicitly extremal non-supersymmetric solutions in the cases in which the attractor mechanism does not completely fix the values of the scalars on the event horizon and they still depend on the boundary conditions at spatial infinity. We compare (su…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsEvent horizonSupergravitySuperpotentialFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyModuli spaceBlack holeCombinatoricsHigh Energy Physics::TheoryGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)AttractorCentral chargeSymplectic geometryJournal of High Energy Physics
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Gauging of flat groups in four dimensional supergravity

2002

We show that N=8 spontaneously broken supergravity in four dimensions obtained by Scherk-Schwarz generalized dimensional reduction can be obtained from a pure four dimensional perspective by gauging a suitable electric subgroup of E_{7,7}. Owing to the fact that there are non isomorphic choices of maximal electric subgroups of the U-duality group their gaugings give rise to inequivalent theories. This in particular shows that the Scherk-Schwarz gaugings do not fall in previous classifications of possible gauged N=8 supergravities. Gauging of flat groups appear in many examples of string compactifications in presence of brane fluxes.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsGroup (mathematics)SupergravityHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesString (physics)Theoretical physicsHigh Energy Physics::TheoryPerspective (geometry)High Energy Physics - Theory (hep-th)Dimensional reductionBraneParticle Physics - Theory
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Aspects of D-brane Dynamics in Supergravity Backgrounds with Fluxes, Kappa-symmetry and Equations of Motion. Part IIB

2006

We derive and carry out a detailed analysis of the equations of motion of the type IIB D branes in generic supergravity backgrounds with fluxes making account of the worldvolume Born-Infeld gauge field and putting a special emphasis on the structure of the Dirac equation for Dp brane fermionic modes. We present an explicit form of the worldvolume field equations for each of the Dp branes (p=1,3,5,7,9) in the cases in which the Neveu-Schwarz flux and the Ramond-Ramond p-form flux along the Dp-brane worldvolume are zero and the supergravity backgrounds do not necessarily induce the worldvolume Born-Infeld flux. We then give several examples of D3, D5 and D7 brane configurations in which the w…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsInstantonCompactification (physics)SupergravityEquations of motionFOS: Physical sciencessymbols.namesakeHigh Energy Physics::TheoryClassical mechanicsHigh Energy Physics - Theory (hep-th)Mathematics::K-Theory and HomologyDirac equationsymbolsBrane cosmologyGauge theoryD-braneMathematical physics
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The two-loop five-particle amplitude in $\mathcal{N}=8$ supergravity

2019

We compute for the first time the two-loop five-particle amplitude in $\mathcal{N}=8$ supergravity. Starting from the known integrand, we perform an integration-by-parts reduction and express the answer in terms of uniform weight master integrals. The latter are known to evaluate to non-planar pentagon functions, described by a 31-letter symbol alphabet. We express the final result for the amplitude in terms of uniform weight four symbols, multiplied by a small set of rational factors. The amplitude satisfies the expected factorization properties when one external graviton becomes soft, and when two external gravitons become collinear. We verify that the soft divergences of the amplitude ex…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsPure mathematics010308 nuclear & particles physicsSupergravityFOS: Physical sciencesFunction (mathematics)01 natural sciencesSmall setScattering amplitudeAmplitudeFactorizationHigh Energy Physics - Theory (hep-th)0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityLimit (mathematics)010306 general physicsScattering AmplitudesSupergravity ModelsN=8 Supergravity
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Q7-branes and their coupling to IIB supergravity

2007

We show how, by making use of a new basis of the IIB supergravity axion-dilaton coset, SL(2,R)/SO(2), 7-branes that belong to different conjugacy classes of the duality group SL(2,R) naturally couple to IIB supergravity with appropriate source terms characterized by an SL(2,R) charge matrix Q. The conjugacy classes are determined by the value of the determinant of Q. The (p,q) 7-branes are the branes in the conjugacy class detQ = 0. The 7-branes in the conjugacy class detQ > 0 are labelled by three numbers (p,q,r) which parameterize the matrix Q and will be called Q7-branes. We construct the full bosonic Wess--Zumino term for the Q7-branes. In order to realize a gauge invariant coupling …

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsPure mathematicsSupergravityFOS: Physical sciencesMONOPOLESInvariant (physics)p-branesBRANESFIELDSINSTANTONSABELIAN BORN-INFELDConjugacy classDOMAIN-WALLSHigh Energy Physics - Theory (hep-th)DUALITYD-branesBrane cosmologyCoset6 DIMENSIONS
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D=11massless superparticle covariant quantization, pure spinor BRST charge and hidden symmetries

2007

We consider the covariant quantization of the D=11 massless superparticle (M0-brane) in the spinor moving frame or twistor-like Lorentz harmonics formulation. The action involves the set of 16 constrained 32 component Majorana spinors, the spinor Lorentz harmonics parametrizing (as homogeneous coordinates, modulo gauge symmetries) the celestial sphere S9. There presence allows us to separate covariantly the first and the second class constraints of the model. After taking into account the second class constraints by means of Dirac brackets and after further reducing the first class constraints algebra, the system is described in terms of a simple BRST charge associated to the d=1, n=16 supe…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsSpinorPure spinorSupergravityFOS: Physical sciencesBRST quantizationCohomologyTwistor theoryHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Quantum mechanicsCovariant transformationSupersymmetry algebraMathematical physicsNuclear Physics B
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Duality and Spontaneously Broken Supergravity in Flat Backgrounds

2002

It is shown that the super Higgs mechanism that occurs in a wide class of models with vanishing cosmological constant (at the classical level) is obtained by the gauging of a flat group which must be an electric subgroup of the duality group. If the residual massive gravitinos which occur in the partial supersymmetry breaking are BPS saturated, then the flat group is non abelian. This is so for all the models obtained by a Scherk-Schwarz supersymmetry breaking mechanism. If gravitinos occur in long multiplets, then the flat groups may be abelian. This is the case of supersymmetry breaking by string compactifications on an orientifold T^6/Z_2 with non trivial brane fluxes.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsSupergravityHigh Energy Physics::PhenomenologyFísicaDuality (optimization)FOS: Physical sciencesSupersymmetry breakingsymbols.namesakeTheoretical physicsHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)OrientifoldsymbolsGravitinoAbelian groupBraneHiggs mechanismParticle Physics - Theory
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N=2 Super-Higgs, N=1 Poincare' Vacua and Quaternionic Geometry

2002

In the context of N=2 supergravity we explain the occurrence of partial super-Higgs with vanishing vacuum energy and moduli stabilization in a model suggested by superstring compactifications on type IIB orientifolds with 3-form fluxes. The gauging of axion symmetries of the quaternionic manifold, together with the use of degenerate symplectic sections for special geometry, are the essential ingredients of the construction.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsSupergravityHigh Energy Physics::PhenomenologySuperstring theoryFOS: Physical sciencesContext (language use)Partícules (Física nuclear)ModuliHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Homogeneous spaceHiggs bosonAxionMathematics::Symplectic GeometryParticle Physics - TheorySymplectic geometryMathematical physics
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Lorentz harmonics and superfield action. D=10, N=1 superstring

2000

We propose a new version of the superfield action for a closed D=10, N=1 superstring where the Lorentz harmonics are used as auxiliary superfields. The incorporation of Lorentz harmonics into the superfield action makes possible to obtain superfield constraints of the induced worldsheet supergravity as equations of motion. Moreover, it becomes evident that a so-called 'Wess-Zumino part' of the superfield action is basically a Lagrangian form of the generalized action principle. We propose to use the second Noether theorem to handle the essential terms in the transformation lows of hidden gauge symmetries, which remove dynamical degrees of freedom from the Lagrange multiplier superfield.

High Energy Physics - TheoryPhysicsPhysics and Astronomy (miscellaneous)WorldsheetLorentz transformationSupergravityHigh Energy Physics::PhenomenologySuperstring theoryEquations of motionFOS: Physical sciencesSuperspaceAction (physics)symbols.namesakeHigh Energy Physics::TheoryNonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)symbolsNoether's theoremMathematical physics
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