Search results for "Higgs mechanism"

showing 10 items of 32 documents

Search for Higgs bosons of the minimal supersymmetric standard model in pp¯ collisions at s=1.96 TeV

2012

We report results from searches for neutral Higgs bosons produced in p-pbar collisions recorded by the Dzero experiment at the Fermilab Tevatron Collider. We study the production of inclusive neutral Higgs boson in the tautau final state and in association with a b quark in the btautau and bbb final states. These results are combined to improve the sensitivity to the production of neutral Higgs bosons in the context of the minimal supersymmetric standard model (MSSM). The data are found to be consistent with expectation from background processes. Upper limits on MSSM Higgs boson production are set for Higgs boson masses ranging from 90 to 300 GeV. We exclude tanBeta>20-30 for Higgs boson ma…

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyElementary particleTechnicolor01 natural sciences7. Clean energyBottom quarkStandard ModelNuclear physicssymbols.namesake0103 physical sciencessymbolsHiggs bosonHigh Energy Physics::Experiment010306 general physicsHiggs mechanismMinimal Supersymmetric Standard ModelBosonPhysics Letters B
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Elementary Goldstone Higgs boson and dark matter

2015

We investigate a perturbative extension of the Standard Model featuring elementary pseudo-Goldstone Higgs and dark matter particles. These are two of the five Goldstone bosons parametrising the SU(4)/Sp(4) coset space. They acquire masses, and therefore become pseudo-Goldstone bosons, due to the embedding of the Yukawa and the electroweak gauge interactions that do not preserve the full SU(4) symmetry. At the one-loop order the top corrections dominate and align the vacuum in the direction where the Higgs is mostly a pseudo-Goldstone boson. Because of the perturbative and elementary nature of the theory, the quantum corrections are precisely calculable. The remaining pseudo-Goldstone boson …

High Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsHiggs bosonHigh Energy Physics::LatticeFOS: Physical sciencesElementary particleTechnicolor01 natural sciencesdark matterStandard Modelsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosons0103 physical sciences010306 general physicsCondensed Matter::Quantum GasesPhysicsGauge bosonta114relic densityelectroweak interaction010308 nuclear & particles physicshep-thHigh Energy Physics::Phenomenologyhep-phHigh Energy Physics - PhenomenologyHiggs fieldscalar particleHigh Energy Physics - Theory (hep-th)symbolsHiggs bosonLHCHiggs mechanismMinimal Supersymmetric Standard ModelPhysical Review D
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Subleading Regge limit from a soft anomalous dimension

2018

Wilson lines capture important features of scattering amplitudes, for example soft effects relevant for infrared divergences, and the Regge limit. Beyond the leading power approximation, corrections to the eikonal picture have to be taken into account. In this paper, we study such corrections in a model of massive scattering amplitudes in N = 4 super Yang-Mills, in the planar limit, where the mass is generated through a Higgs mechanism. Using known three-loop analytic expressions for the scattering amplitude, we find that the first power suppressed term has a very simple form, equal to a single power law. We propose that its exponent is governed by the anomalous dimension of a Wilson loop w…

High Energy Physics - TheoryNuclear and High Energy PhysicsWilson loopScalar (mathematics)FOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesPower lawSupersymmetric Gauge Theorysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityScattering Amplitudes010306 general physicsMathematical physicsPhysics010308 nuclear & particles physicsEikonal equation16. Peace & justiceWilson ’t Hooft and Polyakov loopsScattering amplitudeHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Theory (hep-th)Computer Science::Mathematical SoftwareExponentsymbolslcsh:QC770-798Higgs mechanismJournal of High Energy Physics
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Tracing symmetries and their breakdown through phases of heterotic (2,2) compactifications

2015

We are considering the class of heterotic $\mathcal{N}=(2,2)$ Landau-Ginzburg orbifolds with 9 fields corresponding to $A_1^9$ Gepner models. We classify all of its Abelian discrete quotients and obtain 152 inequivalent models closed under mirror symmetry with $\mathcal{N}=1,2$ and $4$ supersymmetry in 4D. We compute the full massless matter spectrum at the Fermat locus and find a universal relation satisfied by all models. In addition we give prescriptions of how to compute all quantum numbers of the 4D states including their discrete R-symmetries. Using mirror symmetry of rigid geometries we describe orbifold and smooth Calabi-Yau phases as deformations away from the Landau-Ginzburg Ferma…

High Energy Physics - TheoryPhysicsHeterotic string theoryNuclear and High Energy Physics010308 nuclear & particles physicsFOS: Physical sciencesTorusSupersymmetry01 natural sciencesHigh Energy Physics::Theorysymbols.namesakeHigh Energy Physics - Theory (hep-th)0103 physical sciencesHomogeneous spacesymbolsAbelian group010306 general physicsMirror symmetryMathematics::Symplectic GeometryHiggs mechanismOrbifoldMathematical physicsJournal of High Energy Physics
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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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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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A search for invisible Higgs bosons produced in e+e- interactions at LEP 2 energies

1999

Searches for HZ production with the Higgs boson decaying into an invisible final state have been performed with the data collected by the DELPHI experiment up to the centre-of-mass energy of 183 GeV. The hadronic and muon pair final states of the Z boson were analysed. From the absence of signal, upper limits on the cross-section and the corresponding Higgs boson mass limits were set at 95% confidence level. The results are interpreted as excluded parameter regions in the framework of the minimal supersymmetric standard model and in the simplest Majoron model with one Higgs doublet and one Higgs singlet field. (C) 1999 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsParticle physicsCOLLISIONSVIOLATIONSTANDARD MODELMASS01 natural sciencesDECAYSPartícules (Física nuclear)Standard ModelNuclear physicsPHYSICSsymbols.namesakeMONTE-CARLO0103 physical sciencesPROGRAM[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]STANDARD MODEL; MONTE-CARLO; PHYSICS; DECAYS; PROGRAM; SUPERSYMMETRY; COLLISIONS; VIOLATION; PARTICLE; MASS010306 general physicsSUPERSYMMETRYBosonMajoronDELPHIPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySupersymmetryLARGE ELECTRON POSITRON COLLIDERHiggs fieldPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIsymbolsHiggs bosonPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentPARTICLEHiggs mechanismParticle Physics - ExperimentMinimal Supersymmetric Standard Model
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Fully Differential Higgs Pair Production in Association With a $W$ Boson at Next-to-Next-to-Leading Order in QCD

2017

To clarify the electroweak symmetry breaking mechanism, we need to probe the Higgs self-couplings, which can be measured in Higgs pair productions. The associated production with a vector boson is special due to a clear tag in the final state. We perform a fully differential next-to-next-to-leading-order calculation of the Higgs pair production in association with a $W$ boson at hadron colliders, and present numerical results at the 14 TeV LHC and a future 100 TeV hadron collider.

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesTechnicolor01 natural sciencesVector bosonHigh Energy Physics - ExperimentNuclear physicssymbols.namesakeHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::Phenomenologylcsh:QC1-999Higgs fieldHigh Energy Physics - PhenomenologyPair productionsymbolsHiggs bosonHigh Energy Physics::ExperimentHiggs mechanismlcsh:Physics
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Flavour alignment in multi-Higgs-doublet models

2017

Extended electroweak scalar sectors containing several doublet multiplets require flavour-aligned Yukawa matrices to prevent the appearance at tree level of unwanted flavour- changing neutral-current transitions. We analyse the misalignment induced by one-loop quantum corrections and explore possible generalizations of the alignment condition and their compatibility with current experimental constraints. The hypothesis of flavour alignment at a high scale turns out to be consistent with all known phenomenological tests.

Nuclear and High Energy PhysicsParticle physicsHiggs PhysicsHigh Energy Physics::LatticeFlavourFOS: Physical sciences01 natural sciencessymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsMultipletQuantumPhysicsNeutral current010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialHigh Energy Physics - PhenomenologyBeyond Standard ModelsymbolsHiggs bosonlcsh:QC770-798Higgs mechanismJournal of High Energy Physics
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Search for pair production of neutral Higgs bosons in Z$^0$ decays

1990

The pair production of the lightest scalar Higgs boson, h, and a pseudoscalar Higgs boson, A, was searched for in a data sample containing 10 000 hadronic Z0 decays. The search involved both leptonic and purely hadronic decay channels of each Higgs boson. No signal was found, and limits on the Higgs boson masses, in the framework of the minimal supersymmetric extension of the standard model, ar reported up to 35 GeV/c2 at 95% CL, for both tan β > 1 and tan β < 1, where tan β is the ratio of the vacuum expectation values of the two Higgs doublets.

Nuclear and High Energy PhysicsParticle physics[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]Electron–positron annihilationHigh Energy Physics::Lattice01 natural sciencesNuclear physicssymbols.namesake0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsBosonPhysicsCondensed Matter::Quantum Gases010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySupersymmetryScalar bosonPseudoscalarPair productionPhysique des particules élémentairessymbolsHiggs bosonHigh Energy Physics::ExperimentFísica nuclearHiggs mechanismParticle Physics - Experiment
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