Search results for "form factor"

showing 10 items of 261 documents

ISR Experiment at A1-Collaboration

2019

The discrepancy between the proton charge radius extracted from the muonic hydrogen Lamb shift measurement and the best present value obtained from the elastic scattering experiments, remains unexplained and represents a burning problem of today’s nuclear physics. In a pursuit of reconciling the puzzle an experiment is underway at MAMI, which exploits the radiative tail of the elastic peak to study the properties of electromagnetic processes and to extract the proton charge form factor $ \left( {\mathop G\nolimits_E^p } \right) $ at extremely small Q2. This paper reports on the latest results of the first such measurement performed at the three-spectrometer facility of the A1-Collaboration,…

PhysicsElastic scatteringProton010308 nuclear & particles physicsPhysicsQC1-999Form factor (quantum field theory)Charge (physics)01 natural sciencesLamb shiftNuclear physicsCharge radius0103 physical sciencesRadiative transfer010306 general physicsExotic atomEPJ Web of Conferences
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Measurement of the Transverse Beam Spin Asymmetry in Elastic Electron Proton Scattering and the Inelastic Contribution to the Imaginary Part of the T…

2004

We report on a measurement of the asymmetry in the scattering of transversely polarized electrons off unpolarized protons, A$_\perp$, at two Q$^2$ values of \qsquaredaveragedlow (GeV/c)$^2$ and \qsquaredaveragedhighII (GeV/c)$^2$ and a scattering angle of $30^\circ < ��_e < 40^\circ$. The measured transverse asymmetries are A$_{\perp}$(Q$^2$ = \qsquaredaveragedlow (GeV/c)$^2$) = (\experimentalasymmetry alulowcorr $\pm$ \statisticalerrorlow$_{\rm stat}$ $\pm$ \combinedsyspolerrorlowalucor$_{\rm sys}$) $\times$ 10$^{-6}$ and A$_{\perp}$(Q$^2$ = \qsquaredaveragedhighII (GeV/c)$^2$) = (\experimentalasymme tryaluhighcorr $\pm$ \statisticalerrorhigh$_{\rm stat}$ $\pm$ \combinedsyspolerrorhi…

PhysicsElastic scatteringProton13.60.Fz 11.30.Er 13.40.Gp010308 nuclear & particles physicsScatteringElectric form factorGeneral Physics and AstronomyFOS: Physical sciencesInelastic scattering01 natural sciencesNuclear physicsScattering amplitudeAmplitude0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentAtomic physicsNuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear ExperimentNuclear Experiment
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Polarized3He targets in medium energy physics at MAMI

2011

Experiments with polarized 3He targets at the Mainz Microtron (MAMI) involve double polarized photoabsorption or the extraction of the electric form factor of the neutron Ge,n via electron scattering, respectively. Polarized 3He with an initial polarization of up to 70% at the experimental areas is provided by a polarizer based on the principle of metastability exchange optical pumping (MEOP). In this article both target setups for the photon- and the electron beamlines will be described and a status of the data analysis will be given.

PhysicsHistoryPhotonElectric form factorElectronPolarizerPolarization (waves)Computer Science ApplicationsEducationlaw.inventionNuclear physicsOptical pumpinglawNeutronNuclear ExperimentMicrotronJournal of Physics: Conference Series
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Measurements ofB→{π,η,η′}lνlBranching Fractions and Determination of|Vub|with Semileptonically TaggedBMesons

2008

We report measurements of branching fractions for the decays B-->Plnu_{l}, where P are the pseudoscalar charmless mesons pi;{-}, pi;{0}, eta and eta;{'}, based on 348 fb;{-1} of data collected with the BABAR detector, using B0 and B+ mesons found in the recoil of a second B meson decaying as B-->D;{(*)}lnu_{l}. Assuming isospin symmetry, we combine pionic branching fractions to obtain B(B;{0}-->pi;{-}l;{+}nu_{l})=(1.54+/-0.17_{(stat)}+/-0.09_{(syst)})x10;{-4}; we find 3.2sigma evidence of the decay B;{+}-->etal;{+}nu_{l} and measure its branching fraction to be (0.64+/-0.20_{(stat)}+/-0.03_{(syst)})x10;{-4}, and determine B(B;{+}-->eta;{'}l;{+}nu_{l})<0.47x10;{-4} to 90% confidence level. U…

PhysicsMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationHigh Energy Physics::PhenomenologyForm factor (quantum field theory)General Physics and Astronomy01 natural sciencesPseudoscalarParticle decayCrystallographyIsospin0103 physical sciencesHigh Energy Physics::ExperimentB mesonNuclear Experiment010306 general physicsPhysical Review Letters
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Electro- and photodisintegration of deuterium

1978

Deuteron break-up by inelastic electron scattering or photoabsorption is discussed with emphasis on effects from meson exchange currents and isobar configurationgurations.

PhysicsMesonNuclear TheoryForm factor (quantum field theory)Virtual particleNuclear physicsDeuteriumPhotodisintegrationPhysics::Atomic and Molecular ClustersIsobarInelastic electron scatteringHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment
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Breakdown of the expansion of finite-size corrections to the hydrogen Lamb shift in moments of charge distribution

2015

We quantify a limitation in the usual accounting of the finite-size effects, where the leading $[(Z\alpha)^4]$ and subleading $[(Z\alpha)^5]$ contributions to the Lamb shift are given by the mean-square radius and the third Zemach moment of the charge distribution. In the presence of any non-smooth behaviour of the nuclear form factor at scales comparable to the inverse Bohr radius, the expansion of the Lamb shift in the moments breaks down. This is relevant for some of the explanations of the "proton size puzzle". We find, for instance, that the de R\'ujula toy model of the proton form factor does not resolve the puzzle as claimed, despite the large value of the third Zemach moment. Withou…

PhysicsNuclear TheoryProtonAtomic Physics (physics.atom-ph)Form factor (quantum field theory)Electric form factorFOS: Physical sciencesRadiusAtomic and Molecular Physics and OpticsPhysics - Atomic PhysicsLamb shiftNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Charge radiusQuantum mechanicsMoment (physics)Atomic physicsBohr radiusPhysical Review A
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Phenomenological applications of rational approximants

2016

We illustrate the powerfulness of Padé approximants (PAs) as a summation method and explore one of their extensions, the so-called quadratic approximant (QAs), to access both space- and (low-energy) time-like (TL) regions. As an introductory and pedagogical exercise, the function [Formula: see text] is approximated by both kind of approximants. Then, PAs are applied to predict pseudoscalar meson Dalitz decays and to extract [Formula: see text] from the semileptonic [Formula: see text] decays. Finally, the [Formula: see text] vector form factor in the TL region is explored using QAs.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsForm factor (quantum field theory)General Physics and AstronomyAstronomy and AstrophysicsVector meson dominanceFunction (mathematics)Space (mathematics)01 natural sciencesPseudoscalar mesonQuadratic equationQuantum electrodynamics0103 physical sciencesPadé approximantHigh Energy Physics::Experiment010306 general physicsMathematical physicsModern Physics Letters A
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Couplings in coupled channels versus wave functions: Application to theX(3872)resonance

2010

We perform an analytical study of the scattering matrix and bound states in problems with many physical coupled channels. We establish the relationship of the couplings of the states to the different channels, obtained from the residues of the scattering matrix at the poles, with the wave functions for the different channels. The couplings basically reflect the value of the wave functions around the origin in coordinate space. In the concrete case of the $X(3872)$ resonance, understood as a bound state of ${D}^{0}{\overline{D}}^{*0}$ and ${D}^{+}{D}^{*\ensuremath{-}}$ (and $c.c.$ From now on, when we refer to ${D}^{0}{\overline{D}}^{*0}$ , ${D}^{+}{D}^{*\ensuremath{-}}$, or $D{\overline{D}}…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsForm factor (quantum field theory)Order (ring theory)Elementary particle01 natural sciencesResonance (particle physics)IsospinQuantum mechanics0103 physical sciencesBound state10. No inequality010306 general physicsWave functionS-matrixPhysical Review D
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Precision electron beam polarimetry for next generation nuclear physics experiments

2018

Polarized electron beams have played an important role in scattering experiments at moderate to high beam energies. Historically, these experiments have been primarily targeted at studying hadronic structure — from the quark contribution to the spin structure of protons and neutrons, to nucleon elastic form factors, as well as contributions to these elastic form factors from (strange) sea quarks. Other experiments have aimed to place constraints on new physics beyond the Standard Model. For most experiments, knowledge of the magnitude of the electron beam polarization has not been a limiting systematic uncertainty, with only moderately precise beam polarimetry requirements. However, a new …

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsScatteringPolarimetryForm factor (quantum field theory)General Physics and AstronomyElectron01 natural sciencesNuclear physics0103 physical sciencesCathode rayPhysics::Accelerator Physics010306 general physicsNucleonElectron scatteringBeam (structure)International Journal of Modern Physics E
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The decays K→πl+l− beyond leading order in the chiral expansion

1998

We present a model-independent analysis of K+→π+l+l− and KS→π0l+l− decays, including K→3π unitarity corrections and a general decomposition of the dispersive amplitude. From the existing data on K+→π+e+e− we predict the ratio R = B(K+→π+μ+μ−)/B(K+→π+e+e−) to be larger than 0.23, in slight disagreement with the recent measurement R = 0.167±0.036. Consequences for the K±→π±e+e− charge asymmetries and for the KL→π0e+e− mode are also discussed.

PhysicsNuclear and High Energy PhysicsAmplitudeUnitarityForm factor (quantum field theory)Analytical chemistryCP violationJournal of High Energy Physics
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