Search results for " phenomenology"

showing 10 items of 3693 documents

Prospects for charged current deep-inelastic scattering off polarized nucleons at a future electron-ion collider

2013

We present a detailed phenomenological study of charged-current-mediated deep-inelastic scattering off longitudinally polarized nucleons at a future Electron-Ion Collider. A new version of the event generator package DJANGOH, extended by capabilities to handle processes with polarized nucleons, is introduced and used to simulate charged current deep-inelastic scattering including QED, QCD, and electroweak radiative effects. We carefully explore the range of validity and the accuracy of the Jacquet-Blondel method to reconstruct the relevant kinematic variables from the measured hadronic final state in charged current events, assuming realistic detector performance parameters. Finally, we est…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionFOS: Physical sciencesPartonDeep inelastic scatteringlaw.inventionNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawHigh Energy Physics::ExperimentNucleonColliderCharged currentEvent generatorPhysical Review D
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Old and new physics interpretations of the NuTeV anomaly

2001

We discuss whether the NuTeV anomaly can be explained, compatibly with all other data, by QCD effects (maybe, if the strange sea is asymmetric, or there is a tiny violation of isospin), new physics in propagators or couplings of the vector bosons (not really), loops of supersymmetric particles (no), dimension six operators (yes, for one specific SU(2)-invariant operator), leptoquarks (not in a minimal way), extra U(1) gauge bosons (maybe: an unmixed Z' coupled to B-3L_mu also increases the muon g-2 by about 10^{-9} and gives a `burst' to cosmic rays above the GZK cutoff).

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonMuonPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyPropagatorFísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IsospinHigh Energy Physics::ExperimentAnomaly (physics)BosonParticle Physics - Phenomenology
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Violation of quark-hadron duality and spectral chiral moments in QCD

2010

We analyze the spectral moments of the V - A two-point correlation function. Using all known short-distance constraints and the most recent experimental data from tau decays, we determine the lowest spectral moments, trying to assess the uncertainties associated with the so-called violations of quark-hadron duality. We have generated a large number of acceptable spectral functions, satisfying all conditions, and have used them to extract the wanted hadronic parameters through a careful statistical analysis. We obtain accurate values for the chi PT couplings L-10 and C-87, and a realistic determination of the dimension six and eight contributions in the operator product expansion, O-6 = (-5.…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHadronDimension (graph theory)Duality (optimization)FísicaFOS: Physical sciencesElementary particleCorrelation function (quantum field theory)Particle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentOperator product expansion
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Hadron structure at small momentum transfer

2008

Giving three examples, the form factors of the nucleon, the polarisability of the charged pion and the interference of the $S_{11}(1535)$ with the $D_{13}(1520)$ excitation of the nucleon in the $\eta p$-decay channel, it is argued that the hadron structure at low momentum transfer is highly significant for studying QCD.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHadronMomentum transferNuclear TheoryStructure (category theory)FOS: Physical sciencesHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNucleonNuclear ExperimentExcitation
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Photon Plus Jet Production in Large-Q2 ep Collisions at Next-to-Leading Order QCD

1999

The production of photons accompanied by jets in large-Q2 deep inelastic ep scattering is calculated in next-to-leading order. We describe how to consistently include contributions from quark-to-photon fragmentation and give numerical results relevant for HERA experiments.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyPhotonHigh Energy Physics - Phenomenology (hep-ph)ScatteringFOS: Physical sciencesHigh Energy Physics::ExperimentHERA
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Pion transverse momentum dependent parton distributions in the Nambu and Jona-Lasinio model

2015

An explicit evaluation of the two pion transverse momentum dependent parton distributions at leading twist is presented, in the framework of the Nambu-Jona Lasinio model with Pauli-Villars regularization. The transverse momentum dependence of the obtained distributions is generated solely by the dynamics of the model. Using these results, the so called generalized Boer-Mulders shift is studied and compared with recent lattice data. The obtained agreement is very encouraging, in particular because no additional parameter has been introduced. A more conclusive comparison would require a precise knowledge of the QCD evolution of the transverse momentum dependent parton distributions under scru…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeDynamics (mechanics)High Energy Physics::PhenomenologyDeep Inelastic ScatteringLattice (group)FOS: Physical sciencesFísicaPartonChiral Lagrangians; Deep Inelastic Scattering; Phenomenological Models; Nuclear and High Energy PhysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionRegularization (physics)Chiral LagrangiansTransverse momentumTwistNuclear ExperimentPhenomenological Models
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The vector form factor at the next-to-leading order in 1/N(C): chiral couplings L9(mu) and C88(mu) - C90(mu)

2010

24 páginas, 3 figuras, 2 tablas.-- arXiv:1011.5771v1.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeForm factor (quantum field theory)Order (ring theory)ResonanceFOS: Physical sciencesFísica1/N ExpansionQCDRenormalizationMomentumHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPion decay constantNuclear ExperimentChiral lagrangians
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The QCD Effective Charge to All Orders

2002

Using the pinch technique, we show how to construct the QCD effective charge to all orders.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsEffective nuclear chargePhysics::Fluid DynamicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Physics::Plasma PhysicsPinchHigh Energy Physics::Experiment
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Origin of the Large Perturbative Corrections to Higgs Production at Hadron Colliders

2008

The very large K-factor for Higgs-boson production at hadron colliders is shown to result from enhanced perturbative corrections of the form (C_A\pi\alpha_s)^n, which arise in the analytic continuation of the gluon form factor to time-like momentum transfer. These terms are resummed to all orders in perturbation theory using the renormalization group. After the resummation, the K-factor for the production of a light Higgs boson at the LHC is reduced to a value close to 1.3.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Drell–Yan processFOS: Physical sciencesGluonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonProduction (computer science)High Energy Physics::ExperimentResummation
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Charm and bottom quark masses from QCD moment sum rules

2002

In this work the charm and bottom quark masses are determined from QCD moment sum rules for the charmonium and upsilon systems. In our analysis we include both the results from non-relativistic QCD and perturbation theory at next-next-to-leading order. For the pole masses we obtain $M_c=1.75\pm 0.15$ GeV and $M_b=4.98\pm 0.125$ GeV. Using the potential-subtracted mass in intermediate steps of the calculation the MS-masses are determined to $m_c(m_c) = 1.19 \pm 0.11$ GeV and $m_b(m_b) = 4.24 \pm 0.10$ GeV.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesBottom quarkAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Moment (physics)B mesonHigh Energy Physics::ExperimentCharm (quantum number)Perturbation theory (quantum mechanics)Astrophysics::Earth and Planetary AstrophysicsNuclear Experiment
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