Search results for "Electroweak interaction"

showing 10 items of 358 documents

Diphoton resonance from a warped extra dimension

2016

We argue that extensions of the Standard Model (SM) with a warped extra dimension, which successfully address the hierarchy and flavor problems of elementary particle physics, can provide an elegant explanation of the 750 GeV diphoton excess recently reported by ATLAS and CMS. A gauge-singlet bulk scalar with ${\cal O}(1)$ couplings to fermions is identified as the new resonance $S$, and the vector-like Kaluza-Klein excitations of the SM quarks and leptons mediate its loop-induced couplings to photons and gluons. The electroweak gauge symmetry almost unambiguously dictates the bulk matter content and hence the hierarchies of the $S\to \gamma\gamma$, $WW$, $ZZ$, $Z\gamma$, $t\bar t$ and dije…

QuarkQuantum chromodynamicsPhysicsParticle physicsNuclear and High Energy Physics010308 nuclear & particles physicsHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFermionScalar boson750 GeV diphoton excess01 natural sciencesHigh Energy Physics - PhenomenologyHiggs fieldHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsJournal of High Energy Physics
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QCD Jets at HERA II.O(? s 2 ) four-jet cross-sections

1989

We present exact expressions for theO(α s 2 ) tree graph four-jet cross-sections in neutral current and charged current deep inelasticep scattering initiated by quarks, antiquarks and gluons including lepton polarization effects. Using helicity amplitudes the partonic cross-sections are given in concise form including all colour, flavour and statistical factors. We explicate the electroweak coupling dependence and state how the partonic cross-sections are folded with the respective parton densities to obtain theep jet cross-sections toO(α s 2 ). We present some numerical results for the neutral current one-photon exchange case. We elaborate on the cut dependence of the jet rates and present…

QuarkQuantum chromodynamicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)Neutral currentHigh Energy Physics::PhenomenologyElectroweak interactionPartonHERAHelicityGluonNuclear physicsHigh Energy Physics::ExperimentEngineering (miscellaneous)Zeitschrift f�r Physik C Particles and Fields
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Heavy quark spin symmetry and heavy baryons: electroweak decays

2010

Heavy quark spin symmetry is discussed in the context of single and doubly heavy baryons. A special attention is paid to the constraints/simplifications that this symmetry imposes on the non-relativistic constituent quark model wave functions and on the b->c semileptonic decays of these hadrons.

QuarkSemileptonic decayParticle physicsNuclear TheoryHigh Energy Physics::LatticeHadronNuclear TheoryFOS: Physical sciencesConstituent quarkContext (language use)01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyFísicaAtomic and Molecular Physics and OpticsSymmetry (physics)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Two-loop electroweak corrections to the ρ parameter beyond the leading approximation

1996

We show that in the framework of the pinch technique the universal part of the $\rho$ parameter can be meaningfully defined, beyond one loop. The universal part so obtained satisfies the crucial requirements of gauge-independence, finiteness, and process-independence, even when subleading contributions of the top quark are included. The mechanism which enforces the aforementioned properties is explained in detail, and several subtle field theoretical issues are discussed. Explicit calculations of the sub-leading two-loop corrections of order $O(G_{\mu}^{2}m^{2}_{t}M_{Z}^{2})$ are carried out in the context of an $SU(2)$ model, with $M_{W}=M_{Z}$, and various intermediate and final results a…

RenormalizationLoop (topology)PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkHigh Energy Physics - PhenomenologyField (physics)Electroweak interactionCurrent algebraOrder (ring theory)FísicaContext (language use)Physical Review D
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Considerations concerning the renormalization of the electroweak sector of the standard model

1990

Abstract Examination of the structure of one-loop corrected amplitudes for arbitrary processes mediated by W, Z and γ in the simple renormalization framework previously discussed by the author, leads to natural choices for the renormalized self-energies and vertex corrections. They satisfy simple renormalization conditions and, as q2 → 0, the W and Z propagators approach the free expressions with a correction of O(αq2/mW2). The renormalization conditions allow us to circumvent certain ambiguities that arise, to O(α2), in current analyses of Δr and κ(q2). A useful simplified form for the Z propagator is presented.

RenormalizationPhysicsNuclear and High Energy PhysicsCurrent (mathematics)Simple (abstract algebra)Quantum electrodynamicsElectroweak interactionStructure (category theory)Vertex (curve)PropagatorMathematical physicsStandard ModelNuclear Physics B
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First-Principles Calculation of Electroweak Box Diagrams from Lattice QCD.

2020

We present the first realistic lattice QCD calculation of the $\gamma W$-box diagrams relevant for beta decays. The nonperturbative low-momentum integral of the $\gamma W$ loop is calculated using a lattice QCD simulation, complemented by the perturbative QCD result at high momenta. Using the pion semileptonic decay as an example, we demonstrate the feasibility of the method. By using domain wall fermions at the physical pion mass with multiple lattice spacings and volumes, we obtain the axial $\gamma W$-box correction to the semileptonic pion decay, $\Box_{\gamma W}^{VA}\big|_{\pi}=2.830(11)_{\mathrm{stat}}(26)_{\mathrm{sys}}\times10^{-3}$, with the total uncertainty controlled at the leve…

Semileptonic decayParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::LatticeFOS: Physical sciencesGeneral Physics and Astronomy53001 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticePionLattice (order)0103 physical sciencesddc:530NeutronNuclear Experiment010306 general physicsPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyElectroweak interactionPerturbative QCDFermionLattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentPhysical review letters
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Bayesian Analysis of a Future Beta Decay Experiment's Sensitivity to Neutrino Mass Scale and Ordering

2021

Bayesian modeling techniques enable sensitivity analyses that incorporate detailed expectations regarding future experiments. A model-based approach also allows one to evaluate inferences and predicted outcomes, by calibrating (or measuring) the consequences incurred when certain results are reported. We present procedures for calibrating predictions of an experiment's sensitivity to both continuous and discrete parameters. Using these procedures and a new Bayesian model of the $\beta$-decay spectrum, we assess a high-precision $\beta$-decay experiment's sensitivity to the neutrino mass scale and ordering, for one assumed design scenario. We find that such an experiment could measure the el…

Semileptonic decaydata analysis methodParticle physicsBayesian probabilityFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Bayesian inferenceBayesian01 natural sciencesMeasure (mathematics)statistics: Bayesianmass: scaleHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesCalibrationneutrino: massSensitivity (control systems)Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsElectroweak InteractionProbability and statisticssemileptonic decaycalibrationsensitivityneutrino: nuclear reactorHigh Energy Physics - Phenomenologymass: calibration[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physics - Data Analysis Statistics and ProbabilityspectralHigh Energy Physics::ExperimentNeutrinoData Analysis Statistics and Probability (physics.data-an)[PHYS.PHYS.PHYS-DATA-AN]Physics [physics]/Physics [physics]/Data Analysis Statistics and Probability [physics.data-an]Symmetries
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First-forbidden transitions in reactor antineutrino spectra

2019

© 2019 American Physical Society. We study the dominant forbidden transitions in the antineutrino spectra of the fission actinides from 4 MeV onward using the nuclear shell model. Through explicit calculation of the shape factor, we show the expected changes in cumulative electron and antineutrino spectra. Relative to the allowed approximation this results in a minor decrease of electron spectra above 4 MeV, whereas an increase of several percent is observed in antineutrino spectra. We show that forbidden transitions dominate the spectral flux for most of the experimentally accessible range. Based on the shell model calculations we attempt a parametrization of forbidden transitions and prop…

Spectral fluxFissionElectron01 natural sciencesSpectral lineydinreaktiot0103 physical sciencesfission010306 general physicsShape factorNuclear Experimentnuclear tests of fundamental interactionsPhysicsRange (particle radiation)ta114010308 nuclear & particles physicsNuclear shell modelneutriinotshell modelfissioelectroweak interactions in nuclear physicsbeta decayAtomic physicsydinfysiikkaParametrizationPhysical Review C
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The anomalous magnetic moment of the muon in the Standard Model

2020

We are very grateful to the Fermilab Directorate and the Fermilab Theoretical Physics Department for their financial and logistical support of the first workshop of the Muon g -2 Theory Initiative (held near Fermilab in June 2017) [123], which was crucial for its success, and indeed for the successful start of the Initiative. Financial support for this workshop was also provided by the Fermilab Distinguished Scholars program, the Universities Research Association through a URA Visiting Scholar award, the Riken Brookhaven Research Center, and the Japan Society for the Promotion of Science under Grant No. KAKEHNHI-17H02906. We thank Shoji Hashimoto, Toru Iijima, Takashi Kaneko, and Shohei Nis…

Standard ModelNuclear Theorymagnetichigher-orderPhysics beyond the Standard ModelGeneral Physics and Astronomynucl-ex01 natural sciencesHigh Energy Physics - ExperimentSubatomär fysikHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Subatomic Physicsquantum electrodynamics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Vacuum polarizationNuclear Experiment (nucl-ex)Nuclear Experimentfundamental constant: fine structurePhysicsQuantum chromodynamicsQEDAnomalous magnetic dipole momentnew physicsJ-PARC LabHigh Energy Physics - Lattice (hep-lat)Electroweak interactionlattice field theoryParticle Physics - Latticehep-phObservableHigh Energy Physics - PhenomenologyNuclear Physics - TheoryParticle Physics - ExperimentParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]nucl-th530 Physicsdispersion relationg-2Lattice field theoryFOS: Physical scienceshep-latnonperturbative[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530Muon magnetic momentNuclear Theory (nucl-th)High Energy Physics - Latticemuonquantum chromodynamics0103 physical sciencesddc:530Nuclear Physics - Experiment010306 general physicsactivity reportperturbation theoryParticle Physics - PhenomenologyMuonmuon: magnetic momentelectroweak interaction[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]hep-ex010308 nuclear & particles physicsvacuum polarization: hadronicHigh Energy Physics::Phenomenologyphoton photon: scatteringanomalous magnetic moment[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentPhysics Reports
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The su(2|1) Model of Electroweak Interactions and Its Connection to NC Geometry

2002

I review the su(2|1) model of electroweak interactions which is essentially based on the super Lie algebra su(2|1), thus incorporating both usual gauge fields and Higgs fields in one generalized Yang-Mills field. Special emphasis is put on the natural appearance of spontaneous symmetry breaking and other appealing features of the model like generation mixing. Also the connection of the model to noncommutative geometry is briefly discussed.

Theoretical physicsField (physics)Quantum electrodynamicsSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyElectroweak interactionLie algebraHiggs bosonNoncommutative geometrySpecial unitary groupMathematicsConnection (mathematics)
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