Search results for "vector [form factor]"

showing 10 items of 770 documents

Strategies for an accurate determination of the X(3872) energy from QCD lattice simulations

2014

We develop a method to determine accurately the binding energy of the X(3872) from lattice data for the DD* interaction. We show that, because of the small difference between the neutral and charged components of the X(3872), it is necessary to distinguish them in the energy levels of the lattice spectrum if one wishes to have a precise determination of the the binding energy of the X(3872). The analysis of the data requires the use of coupled channels. Depending on the number of levels available and the size of the box we determine the precision needed in the lattice energies to finally obtain a desired accuracy in the binding energy.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsLattice energyBinding energyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFísicaVector meson dominanceHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)Lattice gauge theoryAtomic physicsX(3872)
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Odd-intrinsic-parity processes within the Resonance Effective Theory of QCD

2003

19 páginas, 4 figuras.-- arXiv:hep-ph/0306157v1

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFísicaFOS: Physical sciencesVector meson dominance1/N ExpansionIntrinsic parityQCDPseudoscalarHigh Energy Physics - PhenomenologyPionGlobal symmetriesHigh Energy Physics - Phenomenology (hep-ph)Antisymmetric tensorEffective field theoryHigh Energy Physics::ExperimentChiral lagrangians
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Novel nonperturbative approach for radiativeB¯0(B¯s0)→J/ψγdecays

2016

Radiative ${\overline{B}}^{0}({\overline{B}}_{s}^{0})\ensuremath{\rightarrow}J/\ensuremath{\psi}\ensuremath{\gamma}$ decays provide an interesting case to test our understanding of (non)perturbative QCD and eventually to probe physics beyond the standard model. Recently, the LHCb Collaboration reported an upper bound, updating the results of the BABAR Collaboration. Previous theoretical predictions based on QCD factorization or perturbative QCD have shown large variations due to different treatment of nonfactorizable contributions and meson-photon transitions. In this paper, we report on a novel approach to estimate the decay rates, which is based on a recently proposed model for $B$ decays…

Quantum chromodynamicsPhysicsParticle physics010308 nuclear & particles physicsBranching fractionPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyPerturbative QCDVector meson dominance01 natural sciencesFactorization0103 physical sciencesRadiative transferHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Dynamically generated resonances

2010

We study the radiative decay properties of the charmonium-like X, Y and Z mesons generated dynamically from vector meson-vector meson interaction in the framework of a unitarized hiddengauge formalism. In the present work we calculate the one- and two-photon decay widths of the hidden-charm Y (3940), Z(3930) (or X(3915)) and X(4160) mesons in the framework of the vector meson dominance formalism. We obtain good agreement with experiment in case of the two photon width of the X(3915) which we associate with the 2 + resonance that we find at 3922 MeV.

Quantum chromodynamicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)MesonUnitarityFormalism (philosophy)High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyRadiative decayResonanceVector meson dominanceHigh Energy Physics::ExperimentNuclear ExperimentNuclear theory
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Off-forward Matrix Elements in Light-front Hamiltonian QCD

2002

We investigate the off-forward matrix element of the light cone vector operator for a dressed quark state in light-front Hamiltonian perturbation theory. We obtain the corresponding splitting functions in a straightforward way. We show that the end point singularity is canceled by the contribution from the normalization of state. Considering mixing with the gluon operator, we verify the helicity sum rule in perturbation theory. We show that the quark mass effects are suppressed in the plus component of the matrix element but in the transverse component, they are not suppressed. We emphasize that this is a particularity of the off-forward matrix element and is absent in the forward case.

Quantum chromodynamicsPhysicsQuarkNuclear and High Energy PhysicsParticle physicsVector operatorFOS: Physical sciencesHelicitysymbols.namesakeHigh Energy Physics - PhenomenologySingularityHigh Energy Physics - Phenomenology (hep-ph)Light conesymbolsSum rule in quantum mechanicsHamiltonian (quantum mechanics)Mathematical physics
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Exclusive radiative Higgs decays as probes of light-quark Yukawa couplings

2015

We present a detailed analysis of the rare exclusive Higgs-boson decays into a single vector meson and a photon and investigate the possibility of using these processes to probe the light-quark Yukawa couplings. We work with an effective Lagrangian with modified Higgs couplings to account for possible new-physics effects in a model-independent way. The h->V\gamma{} decay rate is governed by the destructive interference of two amplitudes, one of which involves the Higgs coupling to the quark anti-quark pair inside the vector meson. We derive this amplitude at next-to-leading order in \alpha_s using QCD factorization, including the resummation of large logarithmic corrections and accounting f…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHadronYukawa potentialFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentVector mesonResummationJournal of High Energy Physics
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Unified QCD determination of all vector meson coupling constants

1992

Coupling constants of all vector mesons are determined in QCD by means of a new QCD sum-rule method. The results are found to be sensitive to the binding energy (i.e. meson and quark mass differences). For standard values of quark masses we obtainf ϱ=202 MeV,f K*=216 MeV,f D*=212±22 MeV,f B*=138±42 MeV, $$f_{D_s^* } = 238 \pm 21\,MeV$$ and $$f_{B_s^* } = 163 \pm 45\,MeV$$ . Based on this approach the spin-flavour symmetry for the heavy quark systems are also discussed.

QuarkCoupling constantPhysicsQuantum chromodynamicsParticle physicsPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyBinding energySymmetry (physics)Nuclear physicsHigh Energy Physics::ExperimentVector mesonNuclear ExperimentEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Exclusive heavy vector meson production at next-to-leading order in the dipole picture

2021

We calculate exclusive production of a longitudinally polarized heavy vector meson at next-to-leading order in the dipole picture. The large quark mass allows us to separately include both the first QCD correction proportional to the coupling constant $\alpha_s$, and the first relativistic correction suppressed by the quark velocity $v^2$. Both of these corrections are found to be numerically important in $\mathrm{J}/\psi$ production. The results obtained are directly suitable for phenomenological calculations. We also demonstrate how vector meson production provides complementary information to structure function analyses when one extracts the initial condition for the energy evolution of …

QuarkNuclear and High Energy PhysicsParticle physicsCOLLISIONSProtonJ/PSI MESONSQC1-999High Energy Physics::LatticeNuclear TheoryStructure (category theory)FOS: Physical scienceshiukkasfysiikka7. Clean energy01 natural sciences114 Physical sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesInitial value problemVector meson010306 general physicsNUCLEUSPhysicsCoupling constantQuantum chromodynamicskvarkit010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyELECTROPRODUCTIONEVOLUTIONDipoleHigh Energy Physics - PhenomenologyPHOTOPRODUCTIONHigh Energy Physics::Experiment
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Charmed and strange baryon resonances with heavy-quark spin symmetry

2012

We study charmed and strange baryon resonances that are generated dynamically by a unitary baryon-meson coupled-channel model which incorporates heavy-quark spin symmetry. This is accomplished by extending the SU(3) Weinberg-Tomozawa chiral Lagrangian to SU(8) spin-flavor symmetry plus a suitable symmetry breaking. The model produces resonances with negative parity from s-wave interaction of pseudoscalar and vector mesons with $1/2^+$ and $3/2^+$ baryons. Resonances in all the isospin, spin, and strange sectors with one, two, and three charm units are studied. Our results are compared with experimental data from several facilities, such as the CLEO, Belle or BaBar Collaborations, as well as…

QuarkNuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryNuclear TheoryFOS: Physical sciencesMASSPseudoscalar meson01 natural sciencesNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)MESON-EXCHANGE0103 physical sciencesSymmetry breakingVector mesonNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaCHIRAL DYNAMICSCOUPLED-CHANNELLAMBDA(+)(C)BaryonCharmed baryonsHigh Energy Physics - PhenomenologySTATESIsospinHigh Energy Physics::ExperimentPhysical Review D
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Charmed Mesons in Nuclei with Heavy-Quark Spin Symmetry

2012

We study the properties of charmed pseudoscalar and vector mesons in dense matter within a unitary meson-baryon coupled-channel model which incorporates heavy-quark spin symmetry. This is accomplished by extending the SU(3) Weinberg-Tomozawa Lagrangian to SU(8) spin-flavor symmetry and implementing a suitable flavor symmetry breaking. Several resonances with negative parity are generated dynamically by the s-wave interaction between pseudoscalar and vector meson multiplets with $1/2^+$ and $3/2^+$ baryons. Those states are then compared to experimental data as well as theoretical models. Next, Pauli-blocking effects and meson self-energies are introduced in a self-consistent manner to obtai…

QuarkParticle physicsNuclear TheoryMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesUnitary stateNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesVector mesonSymmetry breakingNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaParity (physics)Atomic and Molecular Physics and OpticsPseudoscalarBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentFew-Body Systems
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