Search results for "Electroweak"

showing 10 items of 744 documents

Two-loop pinch technique in the electroweak sector

2002

The generalization of the two-loop Pinch Technique to the Electroweak Sector of the Standard Model is presented. We restrict ourselves to the case of conserved external currents, and provide a detailed analysis of both the charged and neutral sectors. The crucial ingredient for this construction is the identification of the parts discarded during the pinching procedure with well-defined contributions to the Slavnov-Taylor identity satisfied by the off-shell one-loop gauge-boson vertices; the latter are nested inside the conventional two-loop self-energies. It is shown by resorting to a set of powerful identities that the two-loop effective Pinch Technique self-energies coincide with the cor…

PhysicsNuclear and High Energy PhysicsPhotonElectroweak interactionFísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyTheoretical physicssymbols.namesakeFormalism (philosophy of mathematics)High Energy Physics - Phenomenology (hep-ph)symbolsBibliographyPinchFeynman diagramS-matrixMathematical physicsPhysical Review D
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Primakoff scattering for polarized photons or polarized protons

1993

Abstract We present a way to measure the axial coupling of the proton for the neutral strangeness current in coherent π0 production induced by photon-proton scattering. By means of the γ−Z−π0 triangle anomaly, the parity violating asymmetries for polarized photon or polarized proton Primakoff effect filter the couplings so as to leave the proton axial coupling only. We calculate the relevant observables induced by the electroweak interference and give results for regions of energy and Q2 of possible experimental interest. The polarized proton asymmetry is predicted to be 10−6-10−5 when Q2 ∼ 0.1−0.5 GeV2.

PhysicsNuclear and High Energy PhysicsPhotonProtonScatteringmedia_common.quotation_subjectNuclear TheoryElectroweak interactionStrangenessPolarization (waves)AsymmetryNuclear physicsHigh Energy Physics::ExperimentNuclear ExperimentPrimakoff effectmedia_commonPhysics Letters B
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Tests of the Standard Model with Low-Energy Neutrino Beams

2007

We discuss the possibility of using future high--intensity low--energy neutrino beams for precision tests of the Standard Model. In particular we consider the determination of the electroweak mixing angle from elastic and quasi--elastic neutrino--nucleon scattering at a superbeam or $\beta$--beam.

PhysicsNuclear and High Energy PhysicsScatteringElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesAtomic and Molecular Physics and OpticsSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciStandard ModelNuclear physicsHigh Energy Physics - PhenomenologyLow energyHigh Energy Physics - Phenomenology (hep-ph)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentNeutrinoMixing (physics)Beam (structure)
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ELECTROWEAK THEORY AND THE NEUTRINO-MASS AND NEUTRINO-OSCILLATION QUESTIONS

2007

It is shown that both conjectures of neutrino mass and neutrino oscillation can be made really well-grounded within the Standard Model provided that one adopts a recent new version of the electroweak scheme spontaneously giving also a fundamental explanation for the so-called "maximal parity-violation" effect. A crucial role is played by the prediction of two distinct, scalar and pseudoscalar, replicas of (electron, muon, and tau) lepton numbers that could fully account for an actual non-coincidence between neutrino mass-eigenstates and gauge-eigenstates.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsNeutrino oscillationNeutrino theory of lightHigh Energy Physics::PhenomenologyElectroweak interactionGeneral Physics and AstronomyAstronomy and AstrophysicsStandard Modelelementary-fermion masseMeasurements of neutrino speedHigh Energy Physics::Experimentmaximal parity-violation.NeutrinoNeutrino oscillationLepton
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Leptogenesis with conservation of B–L

2012

Abstract We study leptogenesis in the decay of heavy Standard Model singlet fermions which carry lepton number, in a framework without Majorana masses above the electroweak scale. Based on M. C. Gonzalez-Garcia, J. Racker, N. Rius, JHEP 11 (2009) 079.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyLepton numberAtomic and Molecular Physics and OpticsStandard Model (mathematical formulation)MAJORANALeptogenesisHigh Energy Physics::ExperimentElectroweak scaleNeutrinoNuclear Physics B - Proceedings Supplements
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The Seesaw Scale vs Cosmology

2015

We will study the simplest extension of the Standard Model that can account for neutrino masses: the Type-I seesaw. The model introduces a New Physics scale, M, which is often assumed to be much larger than the electroweak scale. However, it is presently unconstrained and the light neutrino masses and mixing can be generated for any value of M above O(eV). Paying special attention to the contribution of the sterile states to Neff as a function of M, we will show that a large part of the M parameter space (8 orders of magnitude) can be excluded thanks to cosmological measurements. The implications for neutrinoless double beta decay will be discussed too.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologySolar neutrino problemSeesaw molecular geometryMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoElectroweak scaleNeutrino oscillationComputer Science::DatabasesNuclear and Particle Physics Proceedings
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Weak magnetic dipole moments in two-Higgs-doublet models

1995

We investigate the effects of the new scalars in a two-Higgs-doublet model on the weak magnetic dipole moments of the fermions at the $Z$ peak. Proportionality of the Yukawa couplings to the fermion masses, and to $\tan{\beta}$, makes such effects more important for the third family, and potentially relevant. For the $\tau$ lepton, the new diagrams are suppressed by $v_\tau = 2 \sin^2 \theta_W - 1/2$, or by powers of $m_\tau/M_Z$, but may still be comparable to the SM electroweak contributions. In contrast, we find that the new contributions for the bottom quark may be much larger than the SM electroweak contributions. These new effects may even compete with the gluonic contribution, if the…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsElectron–positron annihilationHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaFermionBottom quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentLepton
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Limits on Anomalous Top Couplings from Z Pole Physics

1997

We obtain constraints on possible anomalous interactions of the top quark with the electroweak vector bosons arising from the precision measurements at the Z pole. In the framework of $SU(2)_L \otimes U(1)_Y$ chiral Lagrangians, we examine all effective CP-conserving operators of dimension five which induce fermionic currents involving the top quark. We constrain the magnitudes of these anomalous interactions by evaluating their one-loop contributions to the Z pole physics. Our analysis shows that the operators that contribute to the LEP observables get bounds close to the theoretical expectation for their anomalous couplings. We also show that those which break the $SU(2)_C$ custodial symm…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableCustodial symmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Bounded functionBoson
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Status and Prospects of Top-Quark Physics

2009

The top quark is the heaviest elementary particle observed to date. Its large mass of about 173 GeV/c^2 makes the top quark act differently than other elementary fermions, as it decays before it hadronises, passing its spin information on to its decay products. In addition, the top quark plays an important role in higher-order loop corrections to standard model processes, which makes the top quark mass a crucial parameter for precision tests of the electroweak theory. The top quark is also a powerful probe for new phenomena beyond the standard model. During the time of discovery at the Tevatron in 1995 only a few properties of the top quark could be measured. In recent years, since the star…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesElementary particleFermion01 natural sciencesStandard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Nonlinear Sciences::Exactly Solvable and Integrable Systems0103 physical sciencesPhysics::Atomic and Molecular ClustersHigh Energy Physics::Experiment010306 general physics
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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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