Search results for "PARTICLE PHYSICS"

showing 10 items of 6826 documents

Quantum loops in the resonance chiral theory: the vector form factor

2004

27 páginas, 7 figuras.-- arXiv:hep-ph/0407240v1

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Equations of motionPropagatorFOS: Physical sciencesFísica1/N ExpansionResonance (particle physics)QCDRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Chiral lagrangiansQuantumMathematical physics
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Magnetic moments of theΛ(1405)andΛ(1670)resonances

2002

By using techniques of unitarized chiral perturbation theory, where the $\ensuremath{\Lambda}(1405)$ and $\ensuremath{\Lambda}(1670)$ resonances are dynamically generated, we evaluate the magnetic moments of these resonances and their transition magnetic moment. The results obtained here differ appreciably from those obtained with existing quark models. The width for the $\ensuremath{\Lambda}(1670)\ensuremath{\rightarrow}\ensuremath{\Lambda}(1405)\ensuremath{\gamma}$ transition is also evaluated, leading to a branching ratio of the order of $2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}.$

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMagnetic momentBranching fractionOrder (ring theory)LambdaPhysical Review C
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The neutrinoless double beta decay of 76Ge, 82Se, 86Kr, 114Cd, 128, 130Te and 134, 136Xe in the framework of a relativistic quark confinement model

1991

The half-life of the 0+ → 0+ neutrinoless double beta decay is calculated for 76Ge, 82Se, 86Kr, 114Cd, 128, 130Te and 134, 136Xe and the upper limit for the effective neutrino mass of 3.0 eV is deduced from available experimental data. In addition, the contribution of the right-handed charged weak currents to the effective weak hamiltonian is estimated. The relevant parameters attain the values |〈Λ〉| < 4.1 × 10−6 and |〈ν〉| < 6.6 × 10−8. The nucleonic weak current is treated starting from the current quark level and evaluating the quark current using relativistic quark wave functions obtained from a Dirac equation with a harmonic confinement potential. The nuclear matrix elements of the thus…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsCurrent quarkNuclear physicssymbols.namesakeDirac equationDouble beta decaysymbolsHigh Energy Physics::ExperimentColor confinementNeutrinoWave functionRandom phase approximationNuclear Physics A
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Neutrinoless double beta decay in the dualized standard model

2001

The Dualized Standard Model offers a {\it raison d'\^etre} for 3 fermion generations and an explanation for their distinctive mass and mixing patterns, reproducing to a reasonable accuracy the empirical mixing matrix and mass spectrum for both quarks and leptons in terms of just a few parameters. With its parameters thus fixed, the result is a highly predictive framework. In particular, it is shown that it gives explicit parameter-free predictions for neutrinoless double beta decays. For $^{76}Ge$, it predicts a half-life of $10^{28}-10^{30}$ years, which satisfies the present experimental lower bound of $1.8 \times 10^{25}$ years.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesFísicaFermionUpper and lower boundsStandard ModelHigh Energy Physics - PhenomenologyMatrix (mathematics)High Energy Physics - Phenomenology (hep-ph)Double beta decayMixing (physics)LeptonPhysical Review D
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Charmed and Bottom Baryons: a Variational Approach based on Heavy Quark Symmetry

2003

The use of Heavy Quark Symmetry to study bottom and charmed baryons leads to important simplifications of the non-relativistic three body problem, which turns out to be easily solved by a simple variational ansatz. Our simple scheme reproduces previous results (baryon masses, charge and mass radii, $...$) obtained by solving the Faddeev equations with simple non-relativistic quark--quark potentials, adjusted to the light and heavy--light meson spectra. Wave functions, parameterized in a simple manner, are also given and thus they can be easily used to compute further observables. Our method has been also used to find the predictions for strangeness-less baryons of the SU(2) chirally inspire…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsFaddeev equationsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaCharge (physics)BaryonCharmed baryonsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNuclear ExperimentAnsatz
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Hyperspherical harmonic formalism for tetraquarks

2007

5 pages, 2 tables.-- ISI Article Identifier: 000250926800050.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0610124

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsFormalism (philosophy)GeneralizationHigh Energy Physics::LatticeBound statesNuclear TheoryHigh Energy Physics::PhenomenologySystemsFOS: Physical sciencesFísicaAstronomy and AstrophysicsHarmonic (mathematics)Quantum numberAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Symmetric groupSymmetrizationHigh Energy Physics::ExperimentWave functionMathematical physics
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Non-cancellation of electroweak logarithms in high-energy scattering

2014

We study electroweak Sudakov corrections in high energy scattering, and the cancellation between real and virtual Sudakov corrections. Numerical results are given for the case of heavy quark production by gluon collisions involving the rates $gg \to t \bar t, b \bar b, t \bar b W, t \bar t Z, b \bar b Z, t \bar t H, b \bar b H$. Gauge boson virtual corrections are related to real transverse gauge boson emission, and Higgs virtual corrections to Higgs and longitudinal gauge boson emission. At the LHC, electroweak corrections become important in the TeV regime. At the proposed 100 TeV collider, electroweak interactions enter a new regime, where the corrections are very large and need to be re…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonLarge Hadron ColliderScatteringHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical scienceslcsh:QC1-999law.inventionGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawHiggs bosonHigh Energy Physics::ExperimentColliderlcsh:PhysicsPhysics Letters B
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Probing transverse quark polarization via azimuthal asymmetries in leptoproduction.

1997

We consider the leading order result for polarized leptoproduction, putting emphasis on transverse momentum dependent effects appearing in azimuthal asymmetries. Measurements of weighted cross sections enable extraction of the distribution of transversely polarized quarks. We focus on the distribution in a longitudinally polarized hadron and estimate the expected asymmetries in leptoproduction.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHadronFOS: Physical sciencesPolarization (waves)AzimuthTransverse planeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Transverse momentumHigh Energy Physics::ExperimentNuclear Experiment
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Quark exchange in deep inelastic scattering

1995

We use a model for baryons that links the constituent structure to the deep inelastic (current) properties. The approach consists in a laboratory partonic description (based on a model of hadron structure), to which a low momentum scaleQ 0 is adscribed, which is evolved to high momenta by means of the renormalization group. A generalization of the model by means of the hadronic quark cluster decomposition, provides a description of the structure functions of nuclei and is the starting point to study the effects that the antisymmetrization at the quark level has on the structure function of a model deuteron. The analysis contains conventional and high momentum partonic components. We next st…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHadronHigh Energy Physics::PhenomenologyNuclear TheoryFísicaRenormalization groupDeep inelastic scatteringBaryonNuclear physicsMomentumsymbols.namesakePauli exclusion principlesymbolsNuclear fusionHigh Energy Physics::ExperimentNuclear ExperimentParticle Physics - Phenomenology
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Lattice-constrained parametrizations of form factors for semileptonic and rare radiative B decays

1997

We describe the form factors for B to rho lepton neutrino and B to K* gamma decays with just two parameters and the two form factors for B to pi lepton neutrino with a further two or three parameters. The parametrizations are consistent with heavy quark symmetry, kinematic constraints and lattice results, which we use to determine the parameters. In addition, we test versions of the parametrizations consistent (or not) with light-cone sum rule scaling relations at q^2=0.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologyhep-latLattice QCD calculationFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsSemileptonic and rare radiative decays of B mesonsHigh Energy Physics - LatticeDetermination of Cabibbo-Kobayashi-Maskawa matrix elementsLattice (order)Radiative transferHigh Energy Physics::ExperimentSum rule in quantum mechanicsNeutrinoScalingHeavy quark effective theoryTwo-formLepton
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