Search results for " phenomenology"

showing 10 items of 3693 documents

Lepton flavor violation in the Higgs sector and the role of hadronic tau-lepton decays

2013

It has been pointed out recently that current low-energy constraints still allow for sizable flavor-changing decay rates of the 125 GeV boson into leptons, h -> tau ell (ell= e, mu). In this work we discuss the role of hadronic tau-lepton decays in probing lepton flavor violating couplings in the Higgs sector. At low energy, the effective Higgs coupling to gluons induced by heavy quarks contributes to hadronic tau decays, establishing a direct connection with the relevant process at the LHC, pp (gg)-> h -> tau ell. Semileptonic transitions like tau -> ell pi pi are sensitive to flavor-changing scalar couplings while decays such as tau -> ell eta(') probe pseudoscalar coupling…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesHiggs sectorNuclear physicsPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentConnection (algebraic framework)LeptonBoson
researchProduct

Lattice quark masses: a non-perturbative measurement

1998

We discuss the renormalization of different definitions of quark masses in the Wilson and the tree-level improved SW-Clover fermionic action. For the improved case we give the correct relationship between the quark mass and the hopping parameter. Using perturbative and non-perturbative renormalization constants, we extract quark masses in the $\MSbar$ scheme from Lattice QCD in the quenched approximation at $\beta=6.0$, $\beta=6.2$ and $\beta=6.4$ for both actions. We find: $\bar{m}^{\MSbar}(2 GeV)=5.7 \pm 0.1 \pm 0.8$ MeV, $m_s^{\MSbar}(2GeV)= 130 \pm 2 \pm 18 $ MeV and $m_c^{\MSbar}(2 GeV) = 1662\pm 30\pm 230$ MeV.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice (group)FOS: Physical sciencesFísicaQuenched approximationLattice QCDRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeQCD quark masses latticeBeta (velocity)High Energy Physics::ExperimentNon-perturbativeNuclear ExperimentBar (unit)
researchProduct

Heavy quark mass effects in e+e− into three jets

1998

Next-to-leading order calculation for three jet heavy quark production in e^+e^- collisions, including complete quark mass effects, is reviewed. Its applications at LEP/SLC are also discussed.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaJet (particle physics)Atomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNuclear ExperimentParticle Physics - PhenomenologyNuclear Physics B - Proceedings Supplements
researchProduct

New results from lattice QCD: Non-perturbative renormalization and quark masses

1998

For the first time, we compute non-perturbatively, i.e. without lattice perturbation theory, the renormalization constants of two-fermion operators in the quenched approximation at $\beta=6.0$, 6.2 and 6.4 using the Wilson and the tree-level improved SW-Clover actions. We apply these renormalization constants to fully non-perturbatively estimate quark masses in the $\bar{MS}$ scheme from lattice simulations of both the hadron spectrum and the Axial Ward Identity in the quenched approximation. Some very preliminary unquenched Wilson results obtained from the gluon configurations generated by the T$\chi$L Collaboration at $\beta=5.6$ and $N_{f}=2$ are also discussed.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeLattice (group)FOS: Physical sciencesFísicaQuenched approximationLattice QCDAtomic and Molecular Physics and OpticsGluonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Perturbation theory (quantum mechanics)Non-perturbative
researchProduct

Constraining heavy colored resonances from top-antitop quark events

2009

Recent measurements of the top quark charge asymmetry at Tevatron disfavor the existence of flavor universal axigluons and colorons at 2 sigma. In this letter, we explore the possibility of reconciling the data with these models and use the charge asymmetry and the invariant mass distribution of top-antitop quark pair events to constrain the mass and couplings of massive color-octet gauge bosons decaying to top quarks.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Physics::Atomic and Molecular ClustersEuropean commissionHigh Energy Physics::ExperimentHumanities
researchProduct

Pion parton distributions in a nonlocal Lagrangian

2005

We use phenomenological nonlocal Lagrangians, which lead to non trivial forms for the quark propagator, to describe the pion. We define a procedure, based on the Dyson-Schwinger equations, for the calculation of the pion parton distributions at low Q^2. The obtained parton distributions fulfill all the wishful properties. Using a convolution approach we incorporate the composite character of the constituent quarks in the formalism. We evolve, using the Renormalization Group, the calculated parton distributions to the experimental scale and compare favorably with the data and draw conclusions.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesPropagatorPartonRenormalization groupNon localPartícules (Física nuclear)High Energy Physics - PhenomenologyFormalism (philosophy of mathematics)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)PionsymbolsFísica nuclearHigh Energy Physics::ExperimentNuclear ExperimentLagrangianThe European Physical Journal A
researchProduct

Spectral Functions for Heavy-Light Currents and Form Factor Relations in Hqet

1992

We derive relations among form factors describing the current-induced transitions: (vacuum) $\rightarrow B,B^{*}, B \pi, B^{*} \pi, B \rho$ and $B^{*} \rho$ using heavy quark symmetry. The results are compared to corresponding form factor relations following from identities between scalar and axial vector, and pseudoscalar and vector spectral functions in the heavy quark limit.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyForm factor (quantum field theory)FOS: Physical sciencesSymmetry (physics)PseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Limit (mathematics)Pseudovector
researchProduct

Parton distributions in a constituent quark scenario

1999

A simple picture of the constituent quark as a composite system of point-like partons is used to construct the unpolarized and polarized parton distributions by a convolution between constituent quark momentum distributions and constituent quark structure functions. We achieve good agreement with experiments in the unpolarized, as well as, in the polarized case. When our results are compared with similar calculations using non-composite constituent quarks, the accord with the experiments of the present scheme is impressive. We conclude that DIS data are consistent with a low energy scenario dominated by composite constituents of the nucleon.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeStructure functionNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesConstituent quarkFísicaPartonConvolutionMomentumHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Simple (abstract algebra)High Energy Physics::ExperimentNucleon
researchProduct

New leptoquark mechanism of neutrinoless double beta decay

1996

A new mechanism for neutrinoless double beta ($\znbb$) decay based on leptoquark exchange is discussed. Due to the specific helicity structure of the effective four-fermion interaction this contribution is strongly enhanced compared to the well-known mass mechanism of $\znbb$ decay. As a result the corresponding leptoquark parameters are severely constrained from non-observation of $\znbb$-decay. These constraints are more stringent than those derived from other experiments.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesLepton numberHelicityNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayLeptoquarkBeta (velocity)High Energy Physics::ExperimentNeutrinoLepton
researchProduct

Heavy quark impact factor at next-to-leading order

2000

We further analyze the definition and the calculation of the heavy quark impact factor at next-to-leading (NL) log(s) level, and we provide its analytical expression in a previously proposed k-factorization scheme. Our results indicate that k-factorization holds at NL level with a properly chosen energy scale, and with the same gluonic Green's function previously found in the massless probe case.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsImpact factorScale (ratio)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicahep-phFunction (mathematics)Expression (computer science)Massless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Energy (signal processing)
researchProduct