Search results for "form factor [N(1535)]"

showing 10 items of 205 documents

The η transition form factor from space- and time-like experimental data

2015

The $\eta$ transition form factor is analysed for the first time in both space- and time-like regions at low and intermediate energies in a model-independent approach through the use of rational approximants. The $\eta\rightarrow e^+e^-\gamma$ experimental data provided by the A2 Collaboration in the very low energy region of the dilelectron invariant mass distribution allows for the extraction of the most precise up-to-date slope and curvature parameters of the form factors as well as their values at zero and infinity. The impact of these new results on the mixing parameters of the $\eta$-$\eta^\prime$ system, together with the role played by renormalisation dependent effects, and on the d…

PhysicsPhysics and Astronomy (miscellaneous)Nuclear TheoryAstrophysics::Instrumentation and Methods for AstrophysicsZero (complex analysis)Form factor (quantum field theory)FOS: Physical sciencesComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)CurvatureSpace (mathematics)High Energy Physics - ExperimentNuclear Theory (nucl-th)RenormalizationHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution (mathematics)Computer Science::General LiteratureInvariant massEngineering (miscellaneous)Mixing (physics)Mathematical physics
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Reply to "Comment on `Breakdown of the expansion of finite-size corrections to the hydrogen Lamb shift in moments of charge distribution'"

2016

To comply with the critique of the Comment [J. Arrington, arXiv:1602.01461], we consider another modification of the proton electric form factor, which resolves the "proton-radius puzzle". The proposed modification satisfies all the consistency criteria put forward in the Comment, and yet has a similar impact on the puzzle as that of the original paper. Contrary to the concluding statement of the Comment, it is not difficult to find an ad hoc modification of the form factor at low $Q$ that resolves the discrepancy and is consistent with analyticity constraints. We emphasize once again that we do not consider such an ad hoc modification of the proton form factor to be a solution of the puzzl…

PhysicsProtonNuclear Theory010308 nuclear & particles physicsAtomic Physics (physics.atom-ph)Electric form factorForm factor (quantum field theory)Charge densityFOS: Physical sciencesOf the form01 natural sciencesLamb shiftPhysics - Atomic PhysicsNuclear Theory (nucl-th)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Consistency (statistics)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear theoryNuclear Experiment
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Branching fraction and form-factor shape measurements of exclusive charmless semileptonicBdecays, and determination of|Vub|

2012

We report the results of a study of the exclusive charmless semileptonic decays, B0→π-l+ν, B+→π0l+ν, B+→ωl+ν, B+→ηl+ν, and B+→η′l+ν (l=e or μ) undertaken with approximately 462×106 BB pairs collected at the Υ(4S) resonance with the BABAR detector. The analysis uses events in which the signal B decays are reconstructed with a loose neutrino reconstruction technique. We obtain partial branching fractions in several bins of q2, the square of the momentum transferred to the lepton-neutrino pair, for B0→π-l+ν, B+→π0l+ν, B+→ωl+ν, and B+→ηl+ν. From these distributions, we extract the form-factor shapes f+(q2) and the total branching fractions B(B0→π-l+ν)=(1.45±0.04stat±0.06syst)×10-4 (combined π- …

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionCabibbo–Kobayashi–Maskawa matrixElectron–positron annihilationForm factor (quantum field theory)ResonanceLattice QCD01 natural sciencesNuclear physicsIsospin0103 physical sciences010306 general physicsPhysical Review D
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Measurement of theγγ*→π0transition form factor

2009

We study the reaction e+e- --> e+e-pi0 and measure the gamma gamma* --> pi0 transition form factor in the momentum transfer range from 4 to 40 GeV^2. The analysis is based on 442 fb^-1 of integrated luminosity collected at PEP-II with the BABAR detector at e+e- center-of-mass energies near 10.6 GeV.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsRange (particle radiation)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDetectorMomentum transferForm factor (quantum field theory)Dalitz plot01 natural sciences7. Clean energyMeasure (mathematics)LuminosityNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review D
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The hadronic off-shell width of meson resonances

2000

6 páginas, 4 figuras.-- PACS number(s): 12.39.Fe, 12.38.Aw, 12.38.Cy, 12.40.Vv

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsUnitarityMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryForm factor (quantum field theory)PropagatorFísicaFOS: Physical sciencesVector meson dominanceHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentResummationNuclear Experiment
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Can we understand an auxetic pion-photon transition form factor within QCD?

2013

A state-of-the-art analysis of the pion-photon transition form factor is presented based on an improved theoretical calculation that includes the effect of a finite virtuality of the quasireal photon in the method of light-cone sum rules. We carry out a detailed statistical analysis of the existing experimental data using this method and by employing pion distribution amplitudes with up to three Gegenbauer coefficients a(2), a(4), a(6). Allowing for an error range in the coefficient a(6) approximate to 0, the theoretical predictions for gamma*gamma -> pi(0) obtained with nonlocal QCD sum rules are found to be in good agreement with all data that support a scaling behavior of the transition …

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsQCD sum rulesParticle physicsPhotonForm factor (quantum field theory)Cone Sum-RulesAmplitudePionDistribution (mathematics)Quantum mechanicsQuantum ChromodynamicsHigh Energy Physics::ExperimentScalingPhysical Review D
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A lattice calculation of the hadronic vacuum polarization contribution to (g - 2)μ

2017

We present results of calculations of the hadronic vacuum polarisation contribution to the muon anomalous magnetic moment. Specifically, we focus on controlling the infrared regime of the vacuum polarisation function. Our results are corrected for finite-size effects by combining the Gounaris-Sakurai parameterisation of the timelike pion form factor with the Lüscher formalism. The impact of quark-disconnected diagrams and the precision of the scale determination is discussed and included in our final result in two-flavour QCD, which carries an overall uncertainty of 6%. We present preliminary results computed on ensembles with Nf = 2 + 1 dynamical flavours and discuss how the long-distance …

PhysicsQuantum chromodynamicsParticle physicsMuonAnomalous magnetic dipole moment010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::LatticeHadronHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice (group)Form factor (quantum field theory)FOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesHigh Energy Physics::ExperimentVacuum polarization010306 general physics
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Pseudoscalar transition form factors: (g − 2) of the muon, pseudoscalar decays into lepton pairs, and the η – η′ mixing

2015

We present our model-independent and data-driven method to describe pseudoscalar meson transition form factors in the space- and (low-energy) time-like regions. The method is general and conforms a toolkit applicable to any other form factor, of one and two variables, with the potential to include both high- and low-energy QCD constraints altogether. The method makes use of analyticity and unitary properties of form factors, it is simple, systematic and can be improved upon by including new data. In the present discussion, the method is used to show the impact of experimental data for precision calculations in the low-energy sector of the Standard Model. In particular, due to its relevance …

PhysicsQuantum chromodynamicsParticle physicsMuonNuclear TheoryAnomalous magnetic dipole moment010308 nuclear & particles physicsPhysics beyond the Standard ModelPhysicsQC1-999High Energy Physics::PhenomenologyForm factor (quantum field theory)01 natural sciencesPseudoscalar mesonHigh Energy Physics - ExperimentPseudoscalarHigh Energy Physics - Phenomenology0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLeptonEPJ Web of Conferences
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Rho meson properties in the chiral theory framework

2002

13 páginas, 7 figuras, 1 tabla.-- arXiv:hep-ph/0208199v1

PhysicsQuantum chromodynamicsParticle physicsRho mesonPhysics and Astronomy (miscellaneous)Field (physics)High Energy Physics::PhenomenologyForm factor (quantum field theory)FOS: Physical sciencesOrder (ring theory)ResonanceFísicaQuantum numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Engineering (miscellaneous)Multiplet
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Measurement of theB¯0→D*+ℓ−ν¯ℓdecay rate and|Vcb|

2005

We present a measurement of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$ based on a sample of about 53,700 \mbox{$\Bzb \rightarrow D^{*+} \ell^- \bar{\nu}_{\ell}$} decays observed by the \babar\ detector. We obtain the branching fraction averaged over $\ell = e,\mu$, ${\cal B}(\Bzb \rightarrow D^{*+} \ell^- \bar{\nu}_{\ell}) = (4.90 \pm 0.07\mathrm{(stat.)}^{+0.36}_{-0.35}\mathrm{(syst.)})\%$. We measure the differential decay rate as a function of $w$, the relativistic boost $\gamma$ of the $D^{*+}$ in the ${\Bzb}$ rest frame. By extrapolating $d\Gamma/dw$ to the kinematic limit $w \rightarrow 1$, we extract the product of $|V_{cb}|$ and the axial form factor ${\cal A}_1(w=1)$. …

PhysicsQuantum chromodynamicsSemileptonic decayNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Lattice QCD01 natural sciencesParticle identificationClassical mechanicsProduct (mathematics)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsBar (unit)Physical Review D
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