Search results for "Electroweak interaction"

showing 10 items of 358 documents

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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New Electroweak Formulation Fundamentally Accounting for the Effect Known as “Maximal Parity-Violation”

2006

The electroweak scheme is wholly recast, in the framework of a relativistic quantum field formalism being a covariant fermion–antifermion extension of the usual one for massive spin- $$\frac{1}{2}$$ point fermions. The new formalism is able to reread the “maximal P-violation” effect in a way restoring P and C symmetries themselves: it provides a natural “chiral field” approach, which gives evidence of the existence of a pseudoscalar (extra) charge variety anticommuting with the scalar (ordinary) one and just underlying the “maximally P-violating” phenomenology. Its zero-mass limit leads to a strict “chiral” particle theory, which remodels any massless spin- $$\frac{1}{2}$$ fermion and corre…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)UnitarityHigh Energy Physics::LatticeGeneral MathematicsHigh Energy Physics::PhenomenologyElectroweak interactionParity (physics)FermionPseudoscalarTheoretical physicsHiggs bosonphenomenologyQuantum field theoryorigin of “maximally parity-violatingBosonInternational Journal of Theoretical Physics
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Strongly Coupled Models with a Higgs-like Boson

2013

Considering the one-loop calculation of the oblique S and T parameters, we have presented a study of the viability of strongly-coupled scenarios of electroweak symmetry breaking with a light Higgs-like boson. The calculation has been done by using an effective Lagrangian, being short-distance constraints and dispersive relations the main ingredients of the estimation. Contrary to a widely spread believe, we have demonstrated that strongly coupled electroweak models with massive resonances are not in conflict with experimental constraints on these parameters and the recently observed Higgs-like resonance. So there is room for these models, but they are stringently constrained. The vector and…

PhysicsParticle physicsPhysicsQC1-999Electroweak interactionScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesStandard ModelHigh Energy Physics - PhenomenologyCoupling (physics)High Energy Physics - Phenomenology (hep-ph)Higgs bosonSymmetry breakingSum rule in quantum mechanicsBoson
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R-Parity Breaking in Minimal Supergravity

1999

We consider the Minimal Supergravity Model with universality of scalar and gaugino masses plus an extra bilinear term in the superpotential which breaks R-Parity and lepton number. We explicitly check the consistency of this model with the radiative breaking of the electroweak symmetry. A neutrino mass is radiatively induced, and large Higgs-Lepton mixings are compatible with its experimental bound. We also study briefly the lightest Higgs mass. This one-parameter extension of SUGRA-MSSM is the simplest way of introducing R-parity violation.

PhysicsParticle physicsSupergravityR-parityHigh Energy Physics::PhenomenologyElectroweak interactionGauginoHiggs bosonHigh Energy Physics::ExperimentSupersymmetry breakingLepton numberMinimal Supersymmetric Standard Model
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Perturbative Unitarity Constraints on Charged/Colored Portals

2015

Dark matter that was once in thermal equilibrium with the Standard Model is generally prohibited from obtaining all of its mass from the electroweak or QCD phase transitions. This implies a new scale of physics and mediator particles needed to facilitate dark matter annihilations. In this work, we consider scenarios where thermal dark matter annihilates via scalar mediators that are colored and/or electrically charged. We show how partial wave unitarity places upper bounds on the masses and couplings on both the dark matter and mediators. To do this, we employ effective field theories with dark matter as well as three flavors of sleptons or squarks with minimum flavor violation. For Dirac (…

PhysicsParticle physicsUnitarity010308 nuclear & particles physicsPhysics beyond the Standard ModelDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstronomy and Astrophysics01 natural sciencesUpper and lower boundsStandard ModelMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Space and Planetary Science0103 physical sciencesEffective field theoryHigh Energy Physics::Experiment010306 general physics
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Falsifying High-Scale Leptogenesis at the LHC

2013

Measuring a non-zero value for the cross section of any lepton number violating (LNV) process would put a strong lower limit on the washout factor for the effective lepton number density in the early universe at times close to the electroweak phase transition and thus would lead to important constraints on any high-scale model for the generation of the observed baryon asymmetry based on LNV. In particular, for leptogenesis models with masses of the right-handed neutrinos heavier than the mass scale observed at the LHC, the implied large washout factors would lead to a violation of the out-of-equilibrium condition and exponentially suppress the net lepton number produced in such leptogenesis…

PhysicsPhase transitionParticle physicsLarge Hadron Collidermedia_common.quotation_subjectHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesFísicaGeneral Physics and AstronomyLepton numberUniverseHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Baryon asymmetryLeptogenesisHigh Energy Physics::ExperimentNeutrinomedia_commonPhysical Review Letters
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Supersymmetric electroweak baryogenesis

1999

We calculate the baryon asymmetry generated at the electroweak phase transition in the minimal supersymmetric standard model, using a new method to compute the CP-violating asymmetry in the Higgsino flux reflected into the unbroken phase. The method is based on a Higgs insertion expansion. We find that the CP asymmetry at leading order is proportional to the change in $\tan \beta$ in the bubble wall, which is at most of order $10^{-2}$, while at next-to-leading order this suppression factor disappears. This result may enhance the final baryon asymmetry generated during the electroweak phase transition for small $\Delta \beta (< 10^{-3}$).

PhysicsPhase transitionParticle physicsNuclear and High Energy Physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesFísicaAsymmetryAtomic and Molecular Physics and OpticsBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryHiggs bosonHigh Energy Physics::ExperimentHiggsinoMinimal Supersymmetric Standard Modelmedia_commonNuclear Physics B - Proceedings Supplements
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Lepton asymmetries and primordial hypermagnetic helicity evolution

2012

The hypermagnetic helicity density at the electroweak phase transition (EWPT) exceeds many orders of magnitude the galactic magnetic helicity density. Together with previous magnetic helicity evolution calculations after the EWPT and hypermagnetic helicity conversion to the magnetic one at the EWPT, the present calculation completes the description of the evolution of this important topological feature of cosmological magnetic fields. It suggests that if the magnetic field seeding the galactic dynamo has a primordial origin, it should be substantially helical. This should be taken into account in scenarios of galactic magnetic field evolution with a cosmological seed.

PhysicsPhase transitionParticle physicsQuantitative Biology::BiomoleculesCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsElectroweak interactionFOS: Physical sciencesAstronomy and AstrophysicsAstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesHelicityMagnetic fieldHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)Magnetic helicity0103 physical sciences010306 general physicsDynamoLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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Electroweak baryogenesis at high bubble wall velocities

2020

It is widely believed that electroweak baryogenesis should be suppressed in strong phase transitions with fast-moving bubble walls, but this effect has never been quantitatively studied. We rederive fluid equations describing transport of particle asymmetries near the bubble wall without making the small-wall-velocity approximation. We show that the suppression of the baryon asymmetry is a smooth function of the wall speed and that there is no special behavior when crossing the sound speed barrier. Electroweak baryogenesis can thus be efficient also with strong detonations, generically associated with models with observably large gravitational waves. We also make a systematic and critical c…

PhysicsPhase transitionleptogenesis010308 nuclear & particles physicsGravitational waveBubbleastrofysiikkaElectroweak interactionHigh Energy Physics::Phenomenologybaryogenesishiukkasfysiikkakosmologia01 natural sciences114 Physical sciencesBaryogenesisPhysics::Fluid DynamicsBaryon asymmetryQuantum electrodynamicsSpeed of sound0103 physical sciences010306 general physicsVacuum expectation value
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