Search results for "Weak isospin"

showing 8 items of 8 documents

Parity-violating asymmetry in elastic electron-nucleus scattering due to weak neutral currents

1980

Parity-violating asymmetries are calculated for elastic scattering of electrons on nuclei of arbitrary spin and isospin. Possible dependences on nuclear-model input are shown to be weak. Elastic electron scattering at intermediate energies may become an important tool in studying the structure of hadronic weak neutral currents.

PhysicsElastic scatteringWeak isospinScatteringmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyNuclear TheoryParity (physics)ElectronAsymmetryIsospinQuantum electrodynamicsHigh Energy Physics::ExperimentBorn approximationAtomic physicsNuclear Experimentmedia_commonPhysical Review D
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Weak Interactions and the Standard Model of Strong and Electroweak Interactions

2011

This chapter gives an introduction to the phenomenology and the theory of weak interaction processes involving leptons and hadrons. In Sects. 3.1, 3.2 we collect the most prominent and characteristic properties of weak interactions as they follow from the analysis of a set of key experiments, old and recent. The following sections 3.3–3.5 deal with the elements of non-Abelian local gauge theories in general, and with the unified theory of electroweak and strong interactions of Glashow, Salam and Weinberg (GSW), in particular.

PhysicsGauge bosonTheoretical physicsWeak isospinHigh Energy Physics::PhenomenologyElectroweak interactionHigh Energy Physics::ExperimentGauge theoryWeak interactionUnified field theoryPhenomenology (particle physics)Lepton
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Discriminating between lepton number violating scalars using events with four and three charged leptons at the LHC

2013

Many Standard Model extensions predict doubly-charged scalars; in particular, all models with resonances in charged lepton-pair channels with non-vanishing lepton number; if these are pair produced at the LHC, the observation of their decay into l(-/+)l(-/+)W(-/+)W(-/+) will be necessary in order to establish their lepton-number violating character, which is generally not straightforward. Nonetheless, the analysis of events containing four charged leptons (including scalar decays into one or two taus as well as into W bosons) makes it possible to determine whether the doubly-charged excitation belongs to a multiplet with weak isospin T = 0,1/2,1,3/2 or 2 (assuming there are no excitations w…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderWeak isospinPhysics beyond the Standard ModelAtlas detectorScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLepton numberLeptonNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentMultipletRoot-s=7 tevHadron collidersLeptonBoson
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The decay η → π0h0 in two-higgs-doublet models

1991

The possibility of a light scalar in the framework of two-Higgs-doublet models is studied. The range of masses 100 MeV < mh0 < 2mπ is already excluded by present experiment bounds on the transition η → π0h0 in the model where the neutral component of one doublet couples to fermions with weak isospin T3 = −12 and the neutral component of the second doublet to fermions with T3 = +12. These bounds also constrain tightly the structure of the Yukawa couplings in two-Higgs-doublet models.

PhysicsNuclear and High Energy PhysicsParticle physicsWeak isospinHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyScalar (mathematics)Yukawa potentialElementary particleFermionAtomic and Molecular Physics and OpticsNuclear physicsHiggs fieldsymbols.namesakeHiggs bosonsymbolsHiggs mechanismNuclear Physics B - Proceedings Supplements
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Isospin dependence of the three-nucleon force

2004

We classify $A$--nucleon forces according to their isospin dependence and discuss the most general isospin structure of the three--nucleon force. We derive the leading and subleading isospin--breaking corrections to the three--nucleon force using the framework of chiral effective field theory.

PhysicsNuclear and High Energy PhysicsParticle physicschiral [symmetry]Weak isospinNuclear Theorynuclear forceeffective LagrangianHigh Energy Physics::PhenomenologyNuclear Theorythree-body problem [nucleon]FOS: Physical sciencesFew-body systemsdependence [isospin]Nuclear Theory (nucl-th)Quantum electrodynamicsIsospinEffective field theoryNuclear forceddc:530Symmetry breakingviolation [isospin]Quantum field theoryNucleonNuclear Experiment
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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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Isospin mixing in nuclei within the nuclear density functional theory.

2009

We present the self-consistent, non-perturbative analysis of isospin mixing using the nuclear density functional approach and the rediagonalization of the Coulomb interaction in the good-isospin basis. The largest isospin-breaking effects are predicted for N = Z nuclei and they quickly fall with the neutron excess. The unphysical isospin violation on the mean-field level, caused by the neutron excess, is eliminated by the proposed method. We find a significant dependence of the magnitude of isospin breaking on the parametrization of the nuclear interaction term. A rough correlation has been found between the isospin mixing parameter and the difference of proton and neutron rms radii. The th…

PhysicsParticle physicsWeak isospinProtonNuclear TheoryHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesGeneral Physics and AstronomyNuclear matterNuclear Theory (nucl-th)Nuclear physicsIsospinCoulombNeutronSymmetry breakingNuclear ExperimentNuclear densityPhysical review letters
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Symmetries in the Standard Model

2020

Symmetries in the Physical Laws of Nature lead to observable effects. Beyond the regularities and conserved magnitudes, the last decades in Particle Physics have seen the identification of symmetries, and their well-defined breaking, as the guiding principle for the elementary constituents of matter and their interactions. Flavour SU(3) symmetry of hadrons led to the Quark Model and the antisymmetry requirement under exchange of identical fermions led to the colour degree of freedom. Colour became the generating charge for flavour-independent strong interactions of quarks and gluons in the exact Colour SU(3) local gauge symmetry. Parity violation in weak interactions led to consider the chi…

PhysicsQuarkParticle physicsStandard Model (mathematical formulation)Weak isospinHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyElectroweak interactionHiggs bosonHigh Energy Physics::ExperimentQuantum field theorySymmetry (physics)Gauge symmetry
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