Search results for "Electroweak"

showing 10 items of 744 documents

Tau leptonic branching ratios

1996

A sample of 62249 tau-pair events is selected from data taken with the ALEPH detector in 1991, 1992 and 1993. The measurement of the branching fractions for tau decays into electrons and muons is presented with emphasis on the study of systematic effects from selection, particle identification and decay classification. The results obtained are: B-e=17.79+/-0.12(stat)+/-0.06(syst)(%) and B-mu=17.31+/-0.11(stat)+/-0.05(syst)(%). Combined with the most recent ALEPH determination of the tau lifetime, these results provide a relative measurement of the leptonic couplings in the weak charged current for transverse W bosons: g(mu)/g(e)=1.0002+/-0.0051 and g(tau)/g(mu)=0.9943+/-0.0065. RI ANTONELLI…

PhysicsParticle physicsMuonPhysics and Astronomy (miscellaneous)[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]010308 nuclear & particles physicsElectron–positron annihilationPhysicsElectroweak interaction01 natural sciencesParticle identificationNuclear physicsPositron0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsCharged currentParticle Physics - ExperimentBhabha scatteringBoson
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(g−2)e,μ in an extended inverse type-III seesaw model

2021

There has been a longstanding discrepancy between the experimental measurements of the electron and muon anomalous magnetic moments and their predicted values in the Standard Model. This is particularly relevant in the case of the muon $g\ensuremath{-}2$, which has attracted a remarkable interest in the community after the long-awaited announcement of the first results by the Muon $g\ensuremath{-}2$ collaboration at Fermilab, which confirms a previous measurement by the E821 experiment at Brookhaven and enlarges the statistical significance of the discrepancy, now at $4.2\ensuremath{\sigma}$. In this paper we consider an extension of the inverse type-III seesaw with a pair of vectorlike lep…

PhysicsParticle physicsMuonSeesaw molecular geometryPhysics::Instrumentation and DetectorsInverseHigh Energy Physics::ExperimentElectroweak scaleNeutrinoType (model theory)LeptonStandard ModelPhysical Review D
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The coannihilation codex

2015

We present a general classification of simplified models that lead to dark matter (DM) coannihilation processes of the form DM + X $\rightarrow$ SM$_1$ + SM$_2$, where X is a coannihilation partner for the DM particle and SM$_1$, SM$_2$ are Standard Model fields. Our classification also encompasses regular DM pair annihilation scenarios if DM and X are identical. Each coannhilation scenario motivates the introduction of a mediating particle M that can either belong to the Standard Model or be a new field, whereby the resulting interactions between the dark sector and the Standard Model are realized as tree-level and dimension-four couplings. We construct a basis of coannihilation models, cl…

PhysicsParticle physicsNuclear and High Energy PhysicsAnnihilationLarge Hadron Collider010308 nuclear & particles physicsPhysicsElectroweak interactionDark matterFOS: Physical sciencesFermionQuantum number01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Hadronic CollidersSymmetry breaking010306 general physicsPhenomenological ModelsJournal of High Energy Physics
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Prediction for the lightest Higgs boson mass in the CMSSM using indirect experimental constraints

2007

Measurements at low energies provide interesting indirect information about masses of particles that are (so far) too heavy to be produced directly. Motivated by recent progress in consistently and rigorously calculating electroweak precision observables and flavour related observables, we derive the preferred value for m_h in the Constrained Minimal Supersymmetric Standard Model (CMSSM), obtained from a fit taking into account electroweak precision data, flavour physics observables and the abundance of Cold Dark Matter. No restriction is imposed on m_h itself: the experimental bound from direct Higgs boson search at LEP is not included in the fit. A multi-parameter chi^2 is minimized with …

PhysicsParticle physicsNuclear and High Energy PhysicsCold dark matterHigh Energy Physics::LatticeDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentParticle Physics - ExperimentMinimal Supersymmetric Standard ModelFree parameterParticle Physics - Phenomenology
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Strong phase transition, dark matter and vacuum stability from simple hidden sectors

2014

Motivated by the possibility to explain dark matter abundance and strong electroweak phase transition, we consider simple extensions of the Standard Model containing singlet fields coupled with the Standard Model via a scalar portal. Concretely, we consider a basic portal model consisting of a singlet scalar with $Z_2$ symmetry and a model containing a singlet fermion connected with the Standard Model fields via a singlet scalar portal. We perform a Monte Carlo analysis of the parameter space of each model, and we find that in both cases the dark matter abundance can be produced either via freeze-out or freeze-in mechanisms, but only in the latter model one can obtain also a strong electrow…

PhysicsParticle physicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)ta114Physics beyond the Standard ModelScalar (mathematics)Electroweak interactionDark matterHigh Energy Physics::PhenomenologyeducationFOS: Physical sciences114 Physical sciencesSymmetry (physics)Standard ModelHidden sectorBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityAstrophysics - Cosmology and Nongalactic AstrophysicsNuclear Physics B
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Oblique S and T Constraints on Electroweak Strongly-Coupled Models with a Light Higgs

2014

Using a general effective Lagrangian implementing the chiral symmetry breaking SU(2) L ⊗ SU(2) R → SU(2) L+R , we present a one-loop calculation of the oblique S and T parameters within electroweak strongly-coupled models with a light scalar. Imposing a proper ultraviolet behaviour, we determine S and T at next-to-leading order in terms of a few resonance parameters. The constraints from the global fit to electroweak precision data force the massive vector and axial-vector states to be heavy, with masses above the TeV scale, and suggest that the W + W − and ZZ couplings of the Higgs-like scalar should be close to the Standard Model value. Our findings are generic, since they only rely on so…

PhysicsParticle physicsNuclear and High Energy PhysicsHiggs PhysicsElectroweak interactionScalar (mathematics)High Energy Physics::PhenomenologyOrder (ring theory)Oblique caseFOS: Physical sciencesTechnicolor and Composite ModelsResonance (particle physics)Standard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelHiggs bosonChiral symmetry breakingChiral lagrangians
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A minimal model for ${\rm SU}(N)$ vector dark matter

2015

We study an extension of the Standard Model featuring a hidden sector that consists of a new scalar charged under a new SU$(N)_D$ gauge group, singlet under all Standard Model gauge interactions, and coupled with the Standard Model only via a Higgs portal. We assume that the theory is classically conformal, with electroweak symmetry breaking dynamically induced via the Coleman-Weinberg mechanism operating in the hidden sector. Due to the symmetry breaking pattern, the SU$(N)_D$ gauge group is completely Higgsed and the resulting massive vectors of the hidden sector constitute a stable dark matter candidate. We perform a thorough scan over the parameter space of the model at different values…

PhysicsParticle physicsNuclear and High Energy PhysicsHiggs Physicsta114010308 nuclear & particles physicsElectroweak interactionDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesHiggs physics01 natural sciences114 Physical sciencesStandard ModelMinimal modelHidden sectorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Gauge group0103 physical sciencesBeyond Standard ModelHiggs bosonRADIATIVE-CORRECTIONSSymmetry breaking010306 general physics
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Ultraviolet complete technicolor and Higgs physics at LHC

2015

We construct a Technicolor model which provides masses for the electroweak gauge bosons and for all the Standard Model matter fields. Starting from an ultraviolet complete supersymmetric technicolor, we propose a scenario where all elementary scalars, gauginos, and higgsinos are decoupled at an energy scale substantially higher than the electroweak scale, therefore avoiding the little hierarchy problem of the minimal supersymmetric standard model. The resulting low energy theory has an SU(3) global symmetry whose breaking to SO(3) leads to electroweak symmetry breaking. We study in detail the phenomenology of this theory and demonstrate that it reproduces the present LHC data at the same le…

PhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron Colliderta114Electroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorSupersymmetrysupersymmetric modelsHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityLittle hierarchy problemHigh Energy Physics::ExperimentSymmetry breakingLHCMinimal Supersymmetric Standard Model
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Automated NNLL+NLO Resummation for Jet-Veto Cross Sections

2014

In electroweak-boson production processes with a jet veto, higher-order corrections are enhanced by logarithms of the veto scale over the invariant mass of the boson system. In this paper, we resum these Sudakov logarithms at next-to-next-to-leading logarithmic (NNLL) accuracy and match our predictions to next-to-leading order (NLO) fixed-order results. We perform the calculation in an automated way, for arbitrary electroweak final states and in the presence of kinematic cuts on the leptons produced in the decays of the electroweak bosons. The resummation is based on a factorization theorem for the cross sections into hard functions, which encode the virtual corrections to the boson product…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)530 PhysicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesJet (particle physics)symbols.namesakeHigh Energy Physics - PhenomenologyPair productionHigh Energy Physics - Phenomenology (hep-ph)Weierstrass factorization theoremsymbolsInvariant massHigh Energy Physics::ExperimentResummationEngineering (miscellaneous)Particle Physics - PhenomenologyLeptonBosonEuropean Physical Journal C
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Electroweak interaction in muonic atoms

1992

The parity non-conserving effective neutral current interaction between charged leptons and nucleons is studied in its implications for atomic physics. Present results on heavy electronic atoms are discussed within the standard electroweak theory and beyond. The new features provided by muonic atoms open the way to the nuclear-spin-dependent parity non-conserving effects. Different observables proposed to study these effects in muonic atoms are reviewed.

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)Neutral currentElectroweak interactionHigh Energy Physics::PhenomenologyFísicaParity (physics)ObservableWeak interactionNuclear physicsPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsNucleonEngineering (miscellaneous)Exotic atomLepton
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