Search results for "Vector"

showing 10 items of 2660 documents

Further Comments on a Vanishing Singlet Axial Vector Charge

1998

The recent suggestion of a vanishing flavor-singlet axial charge of nucleon due to a nontrivial vacuum structure is further amplified. A perturbative QCD discussion, applicable for the heavy quark contributions, relates it to the physics of the decoupling theorem. It is also shown that $g_{A}^{0}\simeq 0$ leads to a negative $\eta'$-meson-quark coupling, which has been found to be compatible with the chiral quark model phenomenology.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeQuark modelNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyPerturbative QCDFísicaAstronomy and AstrophysicsDecoupling (cosmology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSinglet stateNucleonNuclear ExperimentPhenomenology (particle physics)Pseudovector
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The $I=1$ pion-pion scattering amplitude and timelike pion form factor from $N_{\rm f} = 2+1$ lattice QCD

2019

The elastic $I=1$ $p$-wave $\pi\pi$ scattering amplitude is calculated together with the isovector timelike pion form factor using lattice QCD with $N_{\rm f}=2+1$ dynamical quark flavors. Wilson clover ensembles generated by the Coordinated Lattice Simulations (CLS) initiative are employed at four lattice spacings down to $a = 0.05\,\mathrm{fm}$, several pion masses down to $m_{\pi} = 200\,\mathrm{MeV}$, and spatial volumes of extent $L = 3.1-5.5\,\mathrm{fm}$. The set of measurements on these ensembles, which is publicly available, enables an investigation of systematic errors due to the finite lattice spacing and spatial volume. The $\pi\pi$ scattering amplitude is fit on each ensemble b…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsIsovector010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCD01 natural sciencesScattering amplitudeHigh Energy Physics - PhenomenologyLattice constantPionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Dispersion relationLattice (order)0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::Experiment010306 general physics
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Multi-hadron spectroscopy in a large physical volume

2017

We demonstrate the efficacy of the stochastic LapH method to treat all-to-all quark propagation on a $N_f = 2+1$ CLS ensemble with large linear spatial extent $L = 5.5$ fm, allowing us to obtain the benchmark elastic isovector p-wave pion-pion scattering amplitude to good precision already on a relatively small number of gauge configurations. These results hold promise for multi-hadron spectroscopy at close-to-physical pion mass with exponential finite-volume effects under control.

PhysicsQuarkParticle physicsIsovector010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::LatticeComputer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryFOS: Physical sciencesGauge (firearms)01 natural sciencesExponential functionScattering amplitudeHigh Energy Physics - LatticePionHadron spectroscopy0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsSpectroscopyEPJ Web of Conferences
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Doubly charmed Ξcc molecular states from meson-baryon interaction

2018

Stimulated by the new experimental LHCb findings associated with the ${\mathrm{\ensuremath{\Omega}}}_{c}$ states, some of which we have described in a previous work as being dynamically generated through meson-baryon interaction, we have extended this approach to make predictions for new ${\mathrm{\ensuremath{\Xi}}}_{cc}$ molecular states in the $C=2$, $S=0$, and $I=1/2$ sector. These states manifest themselves as poles in the solution of the Bethe-Salpeter equation in coupled channels. The kernels of this equation were obtained using general Lagrangians coming from the hidden local gauge symmetry or massive Yang-Mills theory, and the interactions are dominated by the exchange of light vect…

PhysicsQuarkParticle physicsMeson010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::Phenomenology01 natural sciencesPseudoscalar mesonOmegaBaryonPseudoscalar0103 physical sciencesVector mesonNuclear Experiment010306 general physicsRealization (systems)Physical Review D
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High-precision atomic mass measurements for a CKM unitarity test

2013

Abstract The Cabibbo–Kobayashi–Maskawa (CKM) quark-mixing matrix describes the transformation of quarks from weak-force eigenstates to mass eigenstates. The most contributing element in this matrix is the up-down matrix element V ud , derived in most precise way from the nuclear beta decays and in particular, from decays having superallowed 0 +  → 0 + decay branch. What high-precision mass spectrometry community can offer are decay energies of such decays derived from parent–daughter mass differences, which are ideally, and in almost all cases, determined with Penning trap mass spectrometry directly from parent–daughter cyclotron frequency ratio. Typically frequency (and thus mass) ratios a…

PhysicsQuarkParticle physicsta114UnitarityHigh Energy Physics::PhenomenologyCyclotronCondensed Matter PhysicsMass spectrometryPenning trapAtomic masslaw.inventionNuclear physicsMatrix (mathematics)lawHigh Energy Physics::ExperimentPhysical and Theoretical ChemistryInstrumentationSpectroscopyEigenvalues and eigenvectorsInternational Journal of Mass Spectrometry
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Taming the higher power corrections in semileptonic B decays

2016

We study the effect of dimension 7 and 8 operators on inclusive semileptonic B decays and the extraction of |Vcb|. Using moments of semileptonic B decay spectra and information based on the Lowest-Lying State saturation Approximation (LLSA) we perform a global fit of the nonperturbative parameters of the heavy quark expansion including for the first time the O(1/mb^{4,5}) contributions. Higher power corrections appear to have a very small effect on the extraction of |Vcb|, independently of the weight we attribute to the LLSA.

PhysicsQuarkSemileptonic decayNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesState (functional analysis)01 natural sciencesSpectral linelcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Quantum electrodynamics0103 physical sciencesSaturation (graph theory)High Energy Physics::Experiment010306 general physicslcsh:Physics
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On Green's function for cylindrically symmetric fields of polarized radiation

2009

Analytic expressions for Green's function describing the process of transfer of polarized radiation in homogeneous isotropic infinite medium in case of cylindrical symmetry and nonconservative scattering are obtained. The solution is based on the set of systems of Abel integral equations of the first kind obtained using the principle of superposition, and the known expression of Green's function for radiation fields with plane-parallel symmetry. Eigenvalue decompositions for the corresponding matrices of generalized spherical functions are found. Using this result the systems of Abel integral equations are diagonalized, and the final solution is obtained.

PhysicsRadiationIsotropyFunction (mathematics)Integral equationAtomic and Molecular Physics and OpticsSymmetry (physics)symbols.namesakeSuperposition principleGreen's functionsymbolsRadiative transferSpectroscopyEigenvalues and eigenvectorsMathematical physicsJournal of Quantitative Spectroscopy and Radiative Transfer
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Type D vacuum solutions: a new intrinsic approach

2013

We present a new approach to the intrinsic properties of the type D vacuum solutions based on the invariant symmetries that these spacetimes admit. By using tensorial formalism and without explicitly integrating the field equations, we offer a new proof that the upper bound of covariant derivatives of the Riemann tensor required for a Cartan-Karlhede classification is two. Moreover we show that, except for the Ehlers-Kundt's C-metrics, the Riemann derivatives depend on the first order ones, and for the C-metrics they depend on the first order derivatives and on a second order constant invariant. In our analysis the existence of an invariant complex Killing vector plays a central role. It al…

PhysicsRiemann curvature tensorPure mathematicsPhysics and Astronomy (miscellaneous)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Invariant (physics)Upper and lower boundsGeneral Relativity and Quantum Cosmologysymbols.namesakeRiemann hypothesisKilling vector fieldGeneral Relativity and Quantum CosmologyHomogeneous spacesymbolsCovariant transformationField equation
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On the saddle loop bifurcation

1990

It is shown that the set of C∞ (generic) saddle loop bifurcations has a unique modulus of stability γ ≥]0, 1[∪]1, ∞[ for (C0, Cr)-equivalence, with 1≤r≤∞. We mean for an equivalence (x,μ) ↦ (h(x,μ), ϕ(μ)) with h continuous and ϕ of class Cr. The modulus γ is the ratio of hyperbolicity at the saddle point of the connection. Already asking ϕ to be a lipeomorphism forces two saddle loop bifurcations to have the same modulus, while two such bifurcations with the same modulus are (C0,±Identity)-equivalent.

PhysicsSaddle pointMathematical analysisModulusVector fieldBifurcation diagramEngineering physicsBifurcationStable manifoldSaddle
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Reggeized model forηandη′photoproduction

2003

A Reggeized model for $\ensuremath{\eta}$ and ${\ensuremath{\eta}}^{\ensuremath{'}}$ photoproduction on the nucleon is presented. In this model, $t$-channel vector meson exchanges are described in terms of Regge trajectories to comply with the correct high energy behavior. We compare this Reggeized model with an isobar model ($\ensuremath{\eta}$-MAID), where the $t$-channel exchanges are described by $\ensuremath{\rho}$ and $\ensuremath{\omega}$ poles. Both models contain the same resonance contributions, and describe current $\ensuremath{\gamma}p\ensuremath{\rightarrow}\ensuremath{\eta}p$ data up to ${E}_{\ensuremath{\gamma}}^{\text{lab}}=2\phantom{\rule{0.3em}{0ex}}\text{GeV}$ quite well,…

PhysicsScattering cross-sectionNuclear and High Energy PhysicsHigh energyParticle physicsMeson productionIsobarHigh Energy Physics::ExperimentVector mesonNuclear ExperimentNucleonOmegaResonance (particle physics)Physical Review C
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