Search results for "weak interaction"

showing 10 items of 431 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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Predictions for the ${\vec{\Lambda }_b \rightarrow J/\psi ~ \Lambda (1405)}$ Λ b → J / ψ Λ ( 1405 ) decay

2015

We calculate the shape of the [Formula: see text] and [Formula: see text] invariant mass distributions in the [Formula: see text] and [Formula: see text] decays that are dominated by the [Formula: see text] resonance. The weak interaction part is the same for both processes and the hadronization into the different meson-baryon channels in the final state is given by symmetry arguments. The most important feature is the implementation of the meson-baryon final-state interaction using two chiral unitary models from different theoretical groups. Both approaches give a good description of antikaon-nucleon scattering data, the complex energy shift in kaonic hydrogen and the line shapes of [Formu…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)MesonUnitarityKaonic hydrogenQuark modelHigh Energy Physics::PhenomenologyNuclear TheoryElementary particleWeak interaction7. Clean energyHadronizationTheoretical physicsInvariant massHigh Energy Physics::Experimentddc:530Nuclear ExperimentEngineering (miscellaneous)
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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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Weak Interactions and Solar Neutrinos: Testing the Oscillation Hypothesis

1988

Various proposals for understanding the reduced solar neutrino flux in terms of non-standard neutrino propagation properties are briefly reviewed in the context of weak interaction theory. Emphasis is given to neutrino oscillation models which may be tested experimentally, despite the small mass parameter involved. Spontaneous lepton number (and R parity) breaking in supergravity — the supersymmetric doublet Majoron model — solves the solar neutrino problem through matter-enhanced neutrino oscillations. The spectrum of supersymmetric particles is restricted in a way that will be probed by high energy collider experiments. In addition, low energy processes associated with the existence of th…

PhysicsParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoHigh Energy Physics::PhenomenologySolar neutrino problemWeak interactionLepton numberNuclear physicsR-parityHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMajoron
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Absolute neutrino mass and the Dirac/Majorana distinction from the weak interaction of aggregate matter

2020

The 2$\nu$-mediated force has a range of microns, well beyond the atomic scale. The effective potential is built from the t-channel absorptive part of the scattering amplitude and depends on neutrino properties on-shell. We demonstrate that neutral aggregate matter has a weak charge and calculate the matrix of six coherent charges for its interaction with definite-mass neutrinos. Near the range of the potential the neutrino pair is non-relativistic, leading to observable absolute mass and Dirac/Majorana distinction via different r-dependence and violation of the weak equivalence principle.

PhysicsParticle physicsRange (particle radiation)Physics::Instrumentation and DetectorsDirac (software)High Energy Physics::PhenomenologyFOS: Physical sciencesObservableCharge (physics)Weak interactionScattering amplitudeMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)NeutrinoPhysical Review
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Rare weak decays and nuclear structure

2014

Abstract. Weak interactions cause the atomic nuclei to decay via beta and double beta decays. Double beta decays are extremely rare since they are weak-interaction processes of the second order. Also (single) beta decays can be extremely rare. This can be caused by either a large di ff erence between the spins of the initial and final state (the so-called “forbidden” beta decays) or an extremely small Q value (decay energy) of the decay. All these cases are discussed in this article, and particular emphasis is given to the neutrino- less double electron capture on the double beta side of decays. peerReviewed

PhysicsParticle physicsSpinsta114Q valueElectron capturePhysicsQC1-999Nuclear structureweak decaysNuclear physicsDecay energyatomic nucleiAtomic nucleusnuclear structureweak interactionsBeta (velocity)High Energy Physics::ExperimentNeutrinoEPJ Web of Conferences
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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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