Search results for "Interaction"

showing 10 items of 5710 documents

Measurements of the Lineshape of the $Z^{0}$ and Determination of Electroweak Parameters from its Hadronic and Leptonic Decays

1994

Abstract: During the LEP running periods in 1990 and 1991 DELPHI has accumulated approximately 450000 Z0 decays into hadrons and charged leptons. The increased event statistics coupled with improved analysis techniques and improved knowledge of the LEP beam energies permit significantly better measurements of the mass and width of the Z0 resonance. Model independent fits to the cross sections and leptonic forward-backward asymmetries yield the following Z0 parameters: the mass and total width M(Z) = 91.187 +/- 0.009 GeV, GAMMA(Z) = 2.486 +/- 0.012 GeV, the hadronic and leptonic partial widths GAMMA(had) = 1.725 +/- 0.012GeV, GAMMA(l) = 83.01 +/- 0.52 MeV, the invisible width GAMMA(inv) = 51…

Nuclear and High Energy PhysicsParticle physicsElectron–positron annihilationLEP-SLC ENERGIESElementary particle01 natural sciences7. Clean energyPartícules (Física nuclear)PHYSICSNuclear physicsBHABHA SCATTERINGParticle decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSLEP-SLC ENERGIES; RADIATIVE-CORRECTIONS; BHABHA SCATTERING; MASS CORRECTIONS; PHYSICS010306 general physicsDetectors de radiacióDELPHIBhabha scatteringPhysics010308 nuclear & particles physicsPhysicsDELPHI; Z0 resonance; mass corrections; radiative correctionsMathematics::History and OverviewHigh Energy Physics::PhenomenologyElectroweak interactionWeinberg angleMASS CORRECTIONSradiative correctionsZ0 resonanceHiggs bosonHigh Energy Physics::ExperimentParticle Physics - ExperimentLepton
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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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Determining Sneutrino Masses and Physical Implications

2005

In some areas of supersymmetry parameter space, sneutrinos are lighter than the charginos and the next-to-lightest neutralino, and they decay into the invisible neutrino plus lightest-neutralino channel with probability one. In such a scenario they can be searched for in decays of charginos that are pair-produced in e+e- collisions, and in associated sneutrino-chargino production in photon-electron collisions. The sneutrino properties can be determined with high accuracy from the edges of the decay energy spectra in the first case and from threshold scans in the second. In the final part of the report we investigate the mass difference of sneutrinos and charged sleptons between the third an…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesannihilation [electron positron]decay modes [chargino]SO(10) [grand unified theory]Nuclear physicsParticle decayHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrypair production [chargino]interaction [photon electron]Invariant massddc:530numerical calculationsPhysicsmass difference [slepton]High Energy Physics::PhenomenologySuperpartnerSupersymmetryboundary conditionseesaw modelHigh Energy Physics - PhenomenologyPair productionNeutralino(4lepton 2sneutrino) [final state]width [chargino]branching ratio [chargino]High Energy Physics::Experimentassociated production [sneutrino]Neutrinomass spectrum [sneutrino]
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Fingerprints of heavy scales in electroweak effective Lagrangians

2017

The couplings of the electroweak effective theory contain information on the heavy-mass scales which are no-longer present in the low-energy Lagrangian. We build a general effective Lagrangian, implementing the electroweak chiral symmetry breaking $SU(2)_L\otimes SU(2)_R\to SU(2)_{L+R}$, which couples the known particle fields to heavier states with bosonic quantum numbers $J^P=0^\pm$ and $1^\pm$. We consider colour-singlet heavy fields that are in singlet or triplet representations of the electroweak group. Integrating out these heavy scales, we analyze the pattern of low-energy couplings among the light fields which are generated by the massive states. We adopt a generic non-linear realiz…

Nuclear and High Energy PhysicsParticle physicsFísica-Modelos matemáticosHiggs PhysicsFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryFísica matemáticaPartículas (Física nuclear)lcsh:Nuclear and particle physics. Atomic energy. RadioactivityElectromagnetismoSymmetry breakingSinglet state010306 general physicsParticles (Nuclear physics)Huellas dactilares.PhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionCromodinámica cuántica.Technicolor and Composite ModelsQuantum numberLagrangian functions.High Energy Physics - PhenomenologyFingerprints.Simetría (Física)Beyond Standard ModelChiral LagrangiansQuantum chromodynamics.Higgs bosonlcsh:QC770-798Chiral symmetry breakingSymmetry (Physics)Lagrange Funciones de.Journal of High Energy Physics
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Pinch technique for Schwinger-Dyson equations

2007

40 pages, 11 figures.-- ISI Article Identifier: 000245922000041.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0611354

Nuclear and High Energy PhysicsParticle physicsGeneralizationStructure (category theory)FOS: Physical sciencesContext (language use)Skeleton (category theory)Theoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Self-energiesBackground-field MethodAbelian Gauge TheoriesPhysicsBackground field methodScalar (physics)FísicaPerturbation-theoryEffective ChargeFundamental interaction3-point VertexHigh Energy Physics - PhenomenologyNonperturbative EffectsQuantum Chromodynamics (QCD)Gauge SymmetryPinchBRST SymmetryJournal of High Energy Physics
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Dynamically generated resonances

2009

In this talk I report on recent work related to the dynamical generation of baryonic resonances, some made up from pseudoscalar meson-baryon, others from vector meson-baryon and a third type from two meson-one baryon systems. We can establish a correspondence with known baryonic resonances, reinforcing conclusions previously drawn and bringing new light on the nature of some baryonic resonances of higher mass.

Nuclear and High Energy PhysicsParticle physicsHidden gauge formalism for vector meson interactionHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsType (model theory)01 natural sciencesWork relatedDynamically generated resonancesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesChiral dynamics010306 general physicsNuclear ExperimentInstrumentationPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaAstronomy and AstrophysicsBaryonPseudoscalarHigh Energy Physics - Phenomenology
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Heavy Higgs of the Twin Higgs models

2018

Twin Higgs models are the prime illustration of neutral naturalness, where the new particles of the twin sector, gauge singlets of the Standard Model (SM), ameliorate the little hierarchy problem. In this work, we analyse phenomenological implications of the heavy Higgs of the Mirror Twin Higgs and Fraternal Twin Higgs models, when electroweak symmetry breaking is linearly realized. The most general structure of twin Higgs symmetry breaking, including explicit soft and hard breaking terms in the scalar potential, is employed. The direct and indirect searches at the LHC are used to probe the parameter space of Twin Higgs models through mixing of the heavy Higgs with the SM Higgs and decays o…

Nuclear and High Energy PhysicsParticle physicsHiggs PhysicsHiggs particle: decayPhysics beyond the Standard ModelHigh Energy Physics::LatticeFOS: Physical scienceselectroweak interaction: spontaneous symmetry breaking01 natural sciencessymmetry: globalStandard ModelFraternal twinHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessymmetry: SU(4)twin Higgs modellcsh:Nuclear and particle physics. Atomic energy. RadioactivitySymmetry breaking010306 general physicsPhysics010308 nuclear & particles physicsGlueballnew physicsElectroweak interactionHigh Energy Physics::PhenomenologyHiggs particle: heavyHigh Energy Physics - PhenomenologyHiggs particle: mass[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Higgs particle: mirror particleBeyond Standard ModelHiggs bosonlcsh:QC770-798[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Little hierarchy problemHigh Energy Physics::ExperimentnaturalnessJournal of High Energy 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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A 125 GeV composite Higgs boson versus flavour and electroweak precision tests

2013

A composite Higgs boson of 125 GeV mass, only mildly fine-tuned, requires top partners with a semi-perturbative coupling and a mass not greater than about a TeV. We analyze the strong constraints on such picture arising from flavour and electroweak precision tests in models of partial compositeness. We consider different representations for the composite fermions and compare the case of an anarchic flavour structure to models with a U(3)^3 and U(2)^3 flavour symmetry. Although non trivially, some models emerge that look capable of accommodating a 125 GeV Higgs boson with top partners in an interesting mass range for discovery at the LHC as well as associated flavour signals.

Nuclear and High Energy PhysicsParticle physicsHiggs bosonHigh Energy Physics::LatticeFlavourHigh Energy Physics. PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHeavy Quark Physics010306 general physicsPhysicsCouplingLarge Hadron Collider010308 nuclear & particles physicsPhysicsElectroweak interactionHigh Energy Physics::PhenomenologyHiggs physicstechnicolor and composite modelsSymmetry (physics)Settore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciHigh Energy Physics - PhenomenologyCP violationComposite fermionBeyond Standard ModelHiggs bosonHigh Energy Physics::ExperimentHeavy Quark Physic
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Supersymmetric type-III seesaw mechanism: Lepton flavor violation and LHC phenomenology

2013

We study a supersymmetric version of the type-III seesaw mechanism considering two variants of the model: a minimal version for explaining neutrino data with only two copies of 24 superfields and a model with three generations of 24-plets. The latter predicts, in general, rates for mu -> e gamma inconsistent with experimental data. However, this bound can be evaded if certain special conditions within the neutrino sector are fulfilled. In the case of two 24-plets, lepton flavor violation constraints can be satisfied much more easily. After specifying the corresponding regions in the minimal supergravity parameter space, we show that under favorable conditions one can test the corresponding …

Nuclear and High Energy PhysicsParticle physicsMassesPhysics beyond the Standard Model01 natural sciences0103 physical sciencesRoot-S=7 tev010306 general physicsRight-handed neutrinosPhysicsLarge Hadron ColliderElectroweak010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionFísicaNon-conservationSupersymmetrySeesaw mechanismUnificationGrand unified theoriesHigh Energy Physics::ExperimentNeutrinoModel higgs-bosonDecaysPhenomenology (particle physics)LeptonStandard model
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