0000000000347124

AUTHOR

M. Morlet

showing 11 related works from this author

Evidence for Strange-Quark Contributions to the Nucleon’s Form Factors atQ2=0.108   (GeV/c)2

2005

We report on a measurement of the parity violating asymmetry in the elastic scattering of polarized electrons off unpolarized protons with the A4 apparatus at MAMI in Mainz at a four momentum transfer value of ${Q}^{2}=0.108\text{ }(\mathrm{GeV}/c{)}^{2}$ and at a forward electron scattering angle of $30\ifmmode^\circ\else\textdegree\fi{}l{\ensuremath{\theta}}_{e}l40\ifmmode^\circ\else\textdegree\fi{}$. The measured asymmetry is ${A}_{LR}(\stackrel{\ensuremath{\rightarrow}}{e}p)=[\ensuremath{-}1.36\ifmmode\pm\else\textpm\fi{}0.29(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}0.13(\mathrm{syst})]\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}$. The expectation from the standard model as…

PhysicsStrange quarkParticle physics010308 nuclear & particles physicsHadronGeneral Physics and AstronomyElementary particleFermionStrangeness01 natural sciencesBaryon0103 physical sciences010306 general physicsNucleonLeptonPhysical Review Letters
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A Monte-Carlo method to analyze the electromagnetic form factors of the nucleon

2007

Parity violating elastic electron-nucleon scattering allows to determine the vector stangeness content of the nucleon. The final uncertainty on the strange form factors is limited, among other parameters, by the uncertainty on the electromagnetic form factors. These are usually fitted with a functional form constrained by boundary conditions at Q 2= 0 and at large Q 2. These conditions induce huge correlations between parameters which are not taken into account to full extent by purely statistical methods. We describe here a Monte-Carlo method which accounts for correlations between parameters to all orders. We also propose a method for taking into account some systematical errors induced b…

PhysicsScatteringMonte Carlo methodParity (physics)Boundary value problemStatistical physicsNucleon
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Study of Two-Photon Exchange via the Beam Transverse Single Spin Asymmetry in Electron-Proton Elastic Scattering at Forward Angles over a Wide Energy…

2020

We report on a new measurement of the beam transverse single spin asymmetry in electron-proton elastic scattering, $A^{ep}_{\perp}$, at five beam energies from 315.1 MeV to 1508.4 MeV and at a scattering angle of $30^{\circ} < \theta < 40^{\circ}$. The covered $Q^2$ values are 0.032, 0.057, 0.082, 0.218, 0.613 (GeV/c)$^2$. The measurement clearly indicates significant inelastic contributions to the two-photon-exchange (TPE) amplitude in the low-$Q^2$ kinematic region. No theoretical calculation is able to reproduce our result. Comparison with a calculation based on unitarity, which only takes into account elastic and $\mathrm{\pi N}$ inelastic intermediate states, suggests that there are ot…

Protonmedia_common.quotation_subjectFOS: Physical sciencesGeneral Physics and AstronomyElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesAsymmetrybeam: energyelectron p: elastic scatteringpi nucleon: intermediate statebenchmark0103 physical scienceseta nucleonpolarization: transverseunitarityNuclear Experiment (nucl-ex)010306 general physicsNuclear Experimentmedia_commonSpin-½PhysicsElastic scatteringexchange: two-photonUnitarityScatteringscattering3. Good healthtransverseintermediate state* Automatic Keywords *kinematicsElementary Particles and FieldsHigh Energy Physics::ExperimentAtomic physicsspin: asymmetryBeam (structure)experimental resultsPhysical Review Letters
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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 $30^\circ &lt; ��_e &lt; 40^\circ$. 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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ProjectileΔand target Roper excitation in thep(d,d′)Xreaction

2000

In this paper we compare a model that contains the mechanisms of $\ensuremath{\Delta}$ excitation in the projectile and Roper excitation in the target with experimental data from two ${(d,d}^{\ensuremath{'}})$ experiments on a proton target. The agreement of the theory with the experiment is fair for the data taken at ${T}_{d}=2.3$ GeV. The $\ensuremath{\Delta}$ excitation in the projectile is predicted close to the observed energy with the correct width. The theory, however, underpredicts by about 40% the cross sections measured at ${T}_{d} = 1.6$ GeV at angles where the cross section has fallen by about two orders of magnitude. The analysis done here allows us to extract an approximate st…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsProjectile01 natural sciencesNuclear physicsCross section (physics)0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsNuclear theoryExcitationEnergy (signal processing)Order of magnitudePhysical Review C
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Measurement of Strange-Quark Contributions to the Nucleon's Form Factors atQ2=0.230   (GeV/c)2

2004

We report on a measurement of the parity-violating asymmetry in the scattering of longitudinally polarized electrons on unpolarized protons at a Q2 of 0.230 (GeV/c)(2) and a scattering angle of theta (e) = 30 degrees - 40 degrees. Using a large acceptance fast PbF2 calorimeter with a solid angle of delta omega = 0.62 sr, the A4 experiment is the first parity violation experiment to count individual scattering events. The measured asymmetry is A(phys)=(-5.44+/-0.54(stat)+/-0.26(sys))x10(-6). The standard model expectation assuming no strangeness contributions to the vector form factors is A(0) = (-6.30+/-0.43) x 10(-6). The difference is a direct measurement of the strangeness contribution t…

PhysicsStrange quarkParticle physicsProton010308 nuclear & particles physicsScatteringHadronGeneral Physics and AstronomyStrangeness01 natural sciencesOmegaNuclear physicsBaryon0103 physical sciences010306 general physicsNucleonPhysical Review Letters
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Real-time calibration of the A4 electromagnetic lead fluoride (PbF2) calorimeter

2011

Abstract Sufficient energy resolution is the key issue for the calorimetry in particle and nuclear physics. The calorimeter of the A4 parity violation experiment at MAMI is a segmented calorimeter where the energy of an event is determined by summing the signals of neighboring channels. In this case, the precise matching of the individual modules is crucial to obtain a good energy resolution. We have developed a calibration procedure for our total absorbing electromagnetic calorimeter which consists of 1022 lead fluoride (PbF 2 ) crystals. This procedure reconstructs the single-module contributions to the events by solving a linear system of equations, involving the inversion of a 1022×1022…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsLead fluorideCalorimetry[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]System of linear equations7. Clean energy01 natural sciencesParticle detectorComputational physicsCalorimeterNuclear physicsElectromagnetic calorimeter0103 physical sciencesMeasuring instrument010306 general physicsInstrumentationBeam (structure)
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Measurement of Strange Quark Contributions to the Vector Form Factors of the Proton atQ2=0.22  (GeV/c)2

2009

A new measurement of the parity violating asymmetry in elastic electron scattering on hydrogen at backward angles and at a four momentum transfer of Q{sup 2}=0.22 (GeV/c){sup 2} is reported here. The measured asymmetry is A{sub LR}=(-17.23{+-}0.82{sub stat}{+-}0.89{sub syst})x10{sup -6}. The standard model prediction assuming no strangeness is A{sub 0}=(-15.87{+-}1.22)x10{sup -6}. In combination with previous results from measurements at forward angles, it is possible to disentangle for the first time the strange form factors at this momentum transfer, G{sub E}{sup s}=0.050{+-}0.038{+-}0.019 and G{sub M}{sup s}=-0.14{+-}0.11{+-}0.11.

PhysicsStrange quarkParticle physicsProton010308 nuclear & particles physicsHadronMomentum transferGeneral Physics and AstronomyElementary particleStrangeness01 natural sciencesBaryonNuclear physics0103 physical sciences010306 general physicsNucleonPhysical Review Letters
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New Measurements of the Beam Normal Spin Asymmetries at Large Backward Angles with Hydrogen and Deuterium Targets

2017

International audience; New measurements of the beam normal single spin asymmetry in the electron elastic and quasielastic scattering on the proton and deuteron, respectively, at large backward angles and at ⟨Q2⟩=0.22  (GeV/c)2 and ⟨Q2⟩=0.35  ( GeV/c)2 are reported. The experimentally observed asymmetries are compared with the theoretical calculation of Pasquini and Vanderhaeghen [Phys. Rev. C 70, 045206 (2004).PRVCAN0556-281310.1103/PhysRevC.70.045206]. The agreement of the measurements with the theoretical calculations shows a dominance of the inelastic intermediate excited states of the nucleon, πN and the Δ resonance. The measurements explore a new, important parameter region of the exc…

Born approximationelectronProtonGeneral Physics and AstronomyElectronelectron nucleonInelastic scattering[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesResonance (particle physics)Nuclear physicsstatistical analysis0103 physical sciencesexcited stateBorn approximation010306 general physicsNuclear ExperimentSpin-½hydrogen: targetPhysicsQuasielastic scatteringexchange: two-photon010308 nuclear & particles physicsnucleoninelastic scatteringangular dependenceresonanceHigh Energy Physics::Experimentdeuteron: targetAtomic physicsNucleonspin: asymmetryexperimental resultsphoton: virtual
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« On-the-go » multispectral imaging system to characterize the development of vineyard foliage

2015

International audience; In Precision Viticulture, multispectral imaging systems are currently used in remote sensing for vineyard vigor characterization but few are employed in proximal sensing. This work presents the potential of a proximal multispectral imaging system mounted on a track-laying tractor equipped with a Greenseeker RT-100 to provide an NDVI index. The camera acquired visible and near-infrared images which were calibrated in reflectance. Vegetation indices were computed and compared to Greenseeker data. From two of the resulting datasets, a spatio-temporal study of foliage description through both optical systems is presented. This first study assessed the proximal imagery re…

0106 biological sciences010104 statistics & probability[INFO.INFO-TS]Computer Science [cs]/Signal and Image Processing[INFO.INFO-TS] Computer Science [cs]/Signal and Image ProcessingNDVImultispectral imagingfoliage characterizationprecision viticulture15. Life on land0101 mathematics01 natural sciencesin-field acquisition010606 plant biology & botany
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Projectile Delta and target Roper excitation in the p(d,d ') X reaction

2000

In this paper we compare a model that contains the mechanisms of Δ excitation in the projectile and Roper excitation in the target with experimental data from two (d, d') experiments on a proton target. The agreement of the theory with the experiment is fair for the data taken at T_d = 2.3 GeV. The Δ excitation in the projectile is predicted close to the observed energy with the correct width. The theory, however, underpredicts by about 40% the cross sections measured at T_d = 1.6 GeV at angles where the cross section has fallen by about two orders of magnitude. The analysis done here allows to extract an approximate strength for the excitation of the Roper [N^*(1440)] excitation and a qual…

Nuclear TheoryFísicaNuclear Experiment
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