Search results for "weak interaction"

showing 10 items of 431 documents

Electroweak Precision Tests of the Standard Model after the Discovery of the Higgs Boson

2019

The global fit of the Standard Model predictions to electroweak precision data, which has been routinely performed in the past decades by several groups, led to the prediction of the top quark and the Higgs boson masses before their respective discoveries. With the measurement of the Higgs boson mass at the Large Hadron Collider (LHC) in 2012 by the ATLAS and CMS collaborations, the last free parameter of the Standard Model of particle physics has been fixed, and the global electroweak fit can be used to test the full internal consistency of the electroweak sector of the Standard Model and constrain models beyond. In this article, we review the current state-of-the-art theoretical calculati…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicshep-exElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical scienceshep-ph01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Internal consistency0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsParticle Physics - ExperimentFree parameterParticle Physics - Phenomenology
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Experimental results on the electroweak interaction

1999

Recent results from the four experiments ALEPH, DELPHI, L3 and OPAL at the Large Electron-Positron collider, LEP at CERN, and by the SLD collaboration at the Stanford Linear Collider, SLC, are reviewed. Analyses from an integrated luminosity of about 150 pb− recorded by each experiment at LEP, taken at different centre-of-mass energies within ±3 GeV around the peak of the Z resonance during the years 1989 to 1995 are available now. Repeated accurate calibrations of the beam energy lead to precise measurements of the mass and of the total width of the Z boson. These results are complemented by measurements at the Z resonance with polarised beams at Stanford. First results from an integrated …

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron ColliderElectron–positron annihilationHigh Energy Physics::PhenomenologyElectroweak interactionTevatronWeinberg angleStandard ModelNuclear physicsHiggs bosonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentProgress in Particle and Nuclear Physics
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Top quark decay in the Aligned two-Higgs-doublet Model

2015

AbstractWe compute the one loop right and left anomalous tensor couplings (gR and gL, respectively) for the top quark, in the aligned two-Higgs-doublet model. They are the magnetic-like couplings in the most general parameterization of the tbW vertex. We find that the aligned two-Higgs doublet model, that includes as particular cases some of the most studied extensions of the Higgs sector, as Type I and II 2HDM, introduces new electroweak contributions and provides theoretical predictions that are very sensitive to both new scalar masses and the neutral scalar mixing angle. The model can account for new CP violation effects via the introduction of complex alignment parameters that have impo…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron ColliderPhysics beyond the Standard ModelElectroweak interactionHigh Energy Physics::PhenomenologyTop quark condensatePartícules (Física nuclear)Two-Higgs-doublet modelsHiggs sectorTwo-Higgs-doublet modelCP violationNew physicsTop anomalous couplings
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Combination of searches for anomalous top quark couplings with 5.4 fb−1 of pp¯ collisions

2012

We present measurements of the tWb coupling form factors using information from electroweak single top quark production and from the helicity of W bosons from top quark decays in t (t) over bar events. We set upper limits on anomalous tWb coupling form factors using data collected with the DO detector at the Tevatron p (p) over bar collider corresponding to an integrated luminosity of 5.4 fb(-1).

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionTevatronTop quark condensate01 natural sciencesHelicitylaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsColliderBosonPhysics Letters B
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Weak-interaction and nuclear-structure aspects of nuclear double beta decay

1998

Abstract Weak-interaction and nuclear-structure aspects of double beta decay are reviewed. Starting from effective electroweak lagrangians, decay rates for the two-neutrino and neutrinoless modes of the nuclear double beta decay transitions are defined and second-order perturbative expressions for the nuclear decay amplitudes are given. Nuclear matrix elements of the relevant operators are presented, as extracted from data and from shell-model and QRPA calculations as well as from other theoretical approximations. The analysis is performed both for the two-neutrino and neutrinoless modes of the decay. The expressions for ground-state-to-ground-state and ground-state-to-excited-state transit…

PhysicsNuclear physicsMatrix (mathematics)Particle physicsDouble beta decayElectroweak interactionNuclear structureGeneral Physics and AstronomyVertex functionHigh Energy Physics::ExperimentWeak interactionRandom phase approximationRadioactive decayPhysics Reports
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Electroweak effects in the extraction of the CKM angle γ from B→Dπ decays

2015

The angle γ of the standard CKM unitarity triangle can be determined from tree-level B-meson decays essentially without hadronic uncertainties. We calculate the second-order electroweak corrections for the B→Dπ modes and show that their impact on the determination of γ could be enhanced by an accidental cancellation of poorly known hadronic matrix elements. However, we do not expect the resulting shift in γ to exceed |δγDπ/γ|≲O(10−4).

PhysicsNuclear physicsParticle physicsMatrix (mathematics)Nuclear and High Energy PhysicsUnitarityExtraction (chemistry)HadronElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experimentlcsh:Physicslcsh:QC1-999Physics Letters B
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Elements of Quantum Electrodynamics and Weak Interactions

2013

Quantum field theory in its application to electroweak and strong interactions has two rather different facets: A pragmatic, empirical one, and an algebraic, systematical one. The pragmatic approach consists in a set of rules and formal calculational procedures which are extremely successful in their application to concrete physical processes, but rest on mathematically shaky ground. The mathematically rigorous approach, in turn, is technically difficult and not very useful, from a practical point of view, for reaching results which can be compared with phenomenology. Generally speaking, quantum field theory quickly becomes rather technical if one wants to understand it in some depth, and g…

PhysicsOpen quantum systemWeak isospinQuantum electrodynamicsElectroweak interactionCavity quantum electrodynamicsBibliographyQuantum field theoryAlgebraic numberPhenomenology (particle physics)
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QEC value of the superallowed β emitter Sc42

2017

Precise measurements of superallowed ${0}^{+}\ensuremath{\rightarrow}{0}^{+}$ $\ensuremath{\beta}$ decay presently provide the most precise value for the weak mixing amplitude ${V}_{u\phantom{\rule{0}{0ex}}d}$. As the largest element of the CKM matrix, ${V}_{u\phantom{\rule{0}{0ex}}d}$ is a critical piece of the Standard Model of the electroweak interaction. The new, precise Penning-trap mass measurement of the decay energy for the superallowed transition in ${}^{42}$Sc opens the door for a much more precise $f\phantom{\rule{0}{0ex}}t$ value determination if its half-life can be measured more precisely as well.

PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixElectroweak interactionValue (computer science)01 natural sciencesMass measurementStandard ModelAmplitudeDecay energy0103 physical sciences010306 general physicsCommon emitterPhysical Review C
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Progress and open questions in the physics of neutrino cross sections at intermediate energies

2014

New and more precise measurements of neutrino cross sections have renewed the interest in a better understanding of electroweak interactions on nucleons and nuclei. This effort is crucial to achieve the precision goals of the neutrino oscillation program, making new discoveries, like the CP violation in the leptonic sector, possible. We review the recent progress in the physics of neutrino cross sections, putting emphasis on the open questions that arise in the comparison with new experimental data. Following an overview of recent neutrino experiments and future plans, we present some details about the theoretical development in the description of (anti)neutrino-induced quasielastic scatter…

PhysicsParticle physics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyNuclear TheoryGeneral Physics and AstronomyStrangeness productionFísica01 natural sciences7. Clean energyPion0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsNucleonNeutrino oscillationNuclear ExperimentEvent (particle physics)
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Consistency of the dynamical high-scale type-I seesaw mechanism

2019

We analyze the consistency of electroweak breaking within the simplest high-scale Standard Model type-I seesaw mechanism. We derive the full two-loop RGEs of the relevant parameters, including the quartic Higgs self-coupling of the Standard Model. For the simplest case of bare "right-handed" neutrino mass terms we find that, with large Yukawa couplings, the Higgs quartic self-coupling becomes negative much below the seesaw scale, so that the model may be inconsistent even as an effective theory. We show, however, that the "dynamical" type-I high-scale seesaw with spontaneous lepton number violation has better stability properties.

PhysicsParticle physics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesType (model theory)01 natural sciencesLepton numberStandard ModelHigh Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physics
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