Search results for "Higgs"

showing 10 items of 1127 documents

Vacuum Induced CP Violation Generating a Complex CKM Matrix with Controlled Scalar FCNC

2018

We propose a viable minimal model with spontaneous CP violation in the framework of a two Higgs doublet model. The model is based on a generalised Branco–Grimus–Lavoura model with a flavoured Z2 symmetry, under which two of the quark families are even and the third one is odd. The lagrangian respects CP invariance, but the vacuum has a CP violating phase, which is able to generate a complex CKM matrix, with the rephasing invariant strength of CP violation compatible with experiment. The question of scalar mediated flavour changing neutral couplings is carefully studied. In particular we point out a deep connection between the generation of a complex CKM matrix from a vacuum phase and the ap…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelScalar (mathematics)FOS: Physical scienceslcsh:Astrophysics01 natural sciencesComputer Science::Digital LibrariesHigh Energy Physics - ExperimentMinimal modelTwo-Higgs-doublet modelHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyHiggs bosonCP violationlcsh:QC770-798High Energy Physics::Experiment
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Direct search for charged Higgs bosons in decays of top quarks

2001

We present a search for charged Higgs bosons in decays of pair-produced top quarks in pbar p collisions at sqrt(s) = 1.8 TeV using 62.2 pb^-1 of data recorded by the D0 detector at the Fermilab Tevatron collider. No evidence is found for signal, and we exclude at 95% confidence most regions of the (M higgs, tan beta) parameter space where the decay t->H b has a branching fraction greater than 0.36 and B(H -> tau nu) is large.

QuarkParticle physicsPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeTevatronFOS: Physical sciencesGeneral Physics and AstronomyParameter space01 natural sciencesHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderBosonPhysics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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Search for the Associated Production of the Standard-Model Higgs Boson in the All-Hadronic Channel

2009

We report on a search for the standard-model Higgs boson in pp collisions at s=1.96 TeV using an integrated luminosity of 2.0 fb(-1). We look for production of the Higgs boson decaying to a pair of bottom quarks in association with a vector boson V (W or Z) decaying to quarks, resulting in a four-jet final state. Two of the jets are required to have secondary vertices consistent with B-hadron decays. We set the first 95% confidence level upper limit on the VH production cross section with V(-> qq/qq('))H(-> bb) decay for Higgs boson masses of 100-150 GeV/c(2) using data from run II at the Fermilab Tevatron. For m(H)=120 GeV/c(2), we exclude cross sections larger than 38 times the standard-m…

QuarkParticle physicsStandardsFinal stateFermilab TevatronHiggs bosonTevatronFOS: Physical sciencesGeneral Physics and AstronomyElementary particleddc:500.201 natural sciences114 Physical sciencesStandard ModelVector bosonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decayTellurium compounds0103 physical sciencesJetsB-hadron decaysHigh energy physics010306 general physicsBosonsBosonStandard-model Higgs bosonsPhysicsIntegrated luminosityHIGGS BOSONModel predictionCross section010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyConfidence levelsUpper limits3. Good healthVector bosonProduction cross sectionBottom quarksSecondary verticesHiggs bosonCDFHigh Energy Physics::Experiment
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From Tree Unitarity to Top Quark Physics in 5D Higgsless Models

2005

In five dimensional models of Higgsless electroweak symmetry breaking, tree level unitarity in gauge boson scattering is restored by the exchange of gauge boson Kaluza-Klein modes instead of a Higgs boson. Unitarity of scattering amplitudes involving top quarks requires also the Kaluza-Klein modes of the third family quarks. It is shown that the relevant unitarity cancellations are consistent with gauge symmetry breaking by boundary conditions. These results are used to constrain the couplings of the top quark to Kaluza-Klein modes and the implications for collider phenomenology are discussed.

QuarkPhysicsCondensed Matter::Quantum GasesHigh Energy Physics - TheoryGauge bosonTop quarkParticle physicsUnitaritySpontaneous symmetry breakingHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorHiggs fieldHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Higgs bosonHigh Energy Physics::Experiment
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Top mass reconstruction in ATLAS

2011

The top-quark mass is a fundamental parameter of the Standard Model. After the discovery of the top quark, the measurements of its properties were of substantial interest. Within the framework of the SM, the top-quark mass can be used in combination with other electroweak precision measurements to constrain the mass of the yet unobserved Higgs boson.\nIn the new era of the Large Hadron Collider (LHC), the first top quarks have been produced in Europe in proton-proton collisions at a center-of-mass energy of 7~TeV. The top-quark mass measurement of ATLAS in the so called lepton+jets channel with 35~pb$^{-1}$ integrated luminosity will be presented. In this early data-taking period the larges…

QuarkPhysicsHistoryTop quarkParticle physicsLarge Hadron ColliderHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyElectroweak interactionTechnicolorTop quark condensateComputer Science ApplicationsEducationNuclear physicsPhysics::Atomic and Molecular ClustersHiggs bosonHigh Energy Physics::ExperimentDetectors and Experimental TechniquesLeptonJournal of Physics: Conference Series
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Review of Particle Properties

2002

This biennial Review summarizes much of Particle Physics. Using data from previous editions, plus 2205 new measurements from 667 papers, we list, evaluate, and average measured properties of gauge bosons, leptons, quarks, mesons, and baryons. We also summarize searches for hypothetical particles such as Higgs bosons, heavy neutrinos, and supersymmetric particles. All the particle properties and search limits are listed in Summary Tables. We also give numerous tables, figures, formulae, and reviews of topics such as the Standard Model, particle detectors, probability, and statistics. This edition features expanded coverage of CP violation in B mesons and of neutrino oscillations. For the fir…

QuarkPhysicsNuclear and High Energy PhysicsGauge bosonParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronElementary particleParticle Data GroupFermion01 natural sciencesStandard Model0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Search for charged Higgs bosons in decays of top quarks

2009

We present a search for charged Higgs bosons in decays of top quarks, in the mass range $80 < m_{H^{\pm} < 155$ GeV, assuming the subsequent decay $H^{+} \to ��^{+} ��_��$ (and its charge conjugate). Using 0.9 fb$^{-1}$ of lepton+jets data collected with the D0 detector at the Fermilab Tevatron $p\bar{p}$ collider, operating at a center of mass energy $\sqrt{s}=1.96$ TeV, we find no evidence for a $H^{\pm}$ signal. Hence, we exclude branching ratios $B(t \to H^+b) > 0.24$ for $m_{H^{\pm}=80$ GeV, and $B(t \to H^+b) > 0.19$ for $m_{H^{\pm}=155$ GeV, at the 95% C.L.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decay0103 physical sciencesHiggs boson[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentFermilab010306 general physicsLeptonBoson
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Quark mixing in the discrete dark matter model

2011

We consider a model in which dark matter is stable as it is charged under a Z2 symmetry that is residual after an A4 flavour symmetry is broken. We consider the possibility to generate the quark masses by charging the quarks appropriately under A4. We find that it is possible to generate the CKM mixing matrix by an interplay of renormalisable and dimension-six operators. In this set-up, we predict the third neutrino mixing angle to be large and the dark matter relic density to be in the correct range. However, low energy observables - in particular meson-antimeson oscillations - strongly limit the available parameter space.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyDark matterFOS: Physical sciences01 natural sciencesStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentB mesonNeutrino010306 general physicsMixing (physics)Nuclear Physics B
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Two-Higgs leptonic minimal flavour violation

2011

We construct extensions of the Standard Model with two Higgs doublets, where there are flavour changing neutral currents both in the quark and leptonic sectors, with their strength fixed by the fermion mixing matrices $V_{CKM}$ and $V_{PMNS}$. These models are an extension to the leptonic sector of the class of models previously considered by Branco, Grimus and Lavoura, for the quark sector. We consider both the cases of Dirac and Majorana neutrinos and identify the minimal discrete symmetry required in order to implement the models in a natural way.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDirac (video compression format)High Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFermion01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsDiscrete symmetry
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Search for charged Higgs bosons in e^{+}e^{-}$ collisions at √s=172 GeV

1998

This paper presents results on charged Higgs boson production, based on LEP data collected at √s = 172 GeV, that complement the previous DELPHI results obtained at centre of mass energies up to 161 GeV. The charged Higgs bosons are assumed to be pair produced and to decay either into a quark pair or into τVτ. The three different possible final states are included in the analysis. Data from ring imaging Cherenkov and microvertex detectors are used to identify the quarks as a cs pair. The number of candidates found is compatible with the background expected from standard processes. Combining the results of the present analysis with those of the previous analysis at lower energies, a new lower…

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectron–positron annihilationHigh Energy Physics::Phenomenology01 natural sciencesNuclear physics0103 physical sciencesLarge Electron–Positron ColliderHiggs bosonHigh Energy Physics::ExperimentLimit (mathematics)010306 general physicsCherenkov radiationComplement (set theory)BosonPhysics letters: B
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