Search results for "waves"

showing 10 items of 1766 documents

Measurement of polarization-transfer to bound protons in carbon and its virtuality dependence

2017

We measured the ratio Px/Pz of the transverse to longitudinal components of polarization transferred from electrons to bound protons in C12 by the C12(e→,e′p→) process at the Mainz Microtron (MAMI). We observed consistent deviations from unity of this ratio normalized to the free-proton ratio, (Px/Pz)C12/(Px/Pz)H1, for both s- and p-shell knocked out protons, even though they are embedded in averaged local densities that differ by about a factor of two. The dependence of the double ratio on proton virtuality is similar to the one for knocked out protons from H2 and He4, suggesting a universal behavior. It further implies no dependence on average local nuclear density.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesElectronPolarization (waves)01 natural scienceslcsh:QC1-999Transverse plane0103 physical sciencesPhysics::Accelerator PhysicsNuclear Experiment (nucl-ex)Atomic physics010306 general physicsNuclear ExperimentMicrotronNuclear Experimentlcsh:PhysicsNuclear density
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Polarization-transfer measurement to a large-virtuality bound proton in the deuteron

2017

Possible differences between free and bound protons may be observed in the ratio of polarization-transfer components, $P'_x/P'_z$. We report the measurement of $P'_x/P'_z$, in the $^2\textrm{H}(\vec{e},e^{\prime}\vec{p})n$ reaction at low and high missing momenta. Observed increasing deviation of $P'_x/P'_z$ from that of a free proton as a function of the virtuality, similar to that observed in \hefour, indicates that the effect in nuclei is due to the virtuality of the knock-out proton and not due to the average nuclear density. The measured differences from calculations assuming free-proton form factors ($\sim10\%$), may indicate in-medium modifications.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesPolarization (waves)01 natural sciencesNATURAL SCIENCES. Physics.lcsh:QC1-999Nuclear physicsPRIRODNE ZNANOSTI. Fizika.Deuterium0103 physical sciencesd(e e’p) ; Electron-scatteringPhysics::Accelerator PhysicsNuclear Experiment (nucl-ex)Electron-scattering010306 general physicsNuclear Experimentd(ee'p)Electron scatteringNuclear ExperimentNuclear densitylcsh:PhysicsPhysics Letters B
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Proton polarization in the p(e,e′p)π0 reaction and the measurement of quadrupole components in the N to Δ transition

1998

The recoil proton polarization in the π0 production off the proton with longitudinally polarized electron beam has been studied as a means to measure quadrupole components in the N to Δ transition. On top of the Δ resonance a high sensitivity to a possible Coulomb quadrupole excitation is found in parallel kinematics. The ratio of S1+/M1+ multipole amplitudes can be determined from the ratio of the two in-scattering-plane recoil proton polarization components. Avoiding the absolute measurement of the polarizations, such a ratio allows small experimental uncertainties. Furthermore, the electron helicity independent proton polarization component enables the characterization of resonant and no…

PhysicsNuclear and High Energy PhysicsProtonNuclear TheoryHadronResonanceElectronPolarization (waves)QuadrupolePhysics::Accelerator PhysicsAtomic physicsNuclear ExperimentMultipole expansionExcitationThe European Physical Journal A
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Study of polarization observables in double pion photoproduction on the proton

2001

Using a model for two pion photoproduction on the proton previously tested in total cross sections and invariant mass distributions, we evaluate here polarization observables on which recent experiments are providing new information. We evaluate cross sections for spin 1/2 and 3/2, which are measured at Mainz and play an important role in tests of the GHD sum rule. We also evaluate the proton polarization asymmetry $\Sigma$ which is currently under investigation at GRAAL in Grenoble.

PhysicsNuclear and High Energy PhysicsProtonNuclear Theorymedia_common.quotation_subjectPolarization observablesNuclear TheoryFísicaFOS: Physical sciencesPolarization (waves)AsymmetryNuclear physicsNuclear Theory (nucl-th)PionInvariant massSum rule in quantum mechanicsNuclear Experimentmedia_commonSpin-½
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Polarization transfer in the 4HeH reaction

2001

Abstract Polarization transfer in the 4He ( e → ,e′ p → ) 3 H reaction at a Q2 of 0.4 (GeV/c)2 was measured at the Mainz Microtron MAMI. The ratio of the transverse to the longitudinal polarization components of the ejected protons was compared with the same ratio for elastic ep scattering. The results are consistent with a recent fully relativistic calculation which includes a predicted medium modification of the proton form factor based on a quark–meson coupling model.

PhysicsNuclear and High Energy PhysicsProtonScatteringNuclear Theorychemistry.chemical_elementPolarization (waves)Nuclear physicsTransverse planechemistryPhysics::Accelerator PhysicsNuclear ExperimentMicrotronHeliumPhysics Letters B
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Production cross-sections and neutron polarization in (p,n) reactions at 143 MeV

1963

Abstract Measurements have been made of the energy spectra and polarizations of neutrons emitted at a laboratory angle of 45° from deuterium, lithium and aluminium bombarded by protons of 143 MeV. The results are consistent with the view that neutron production from deuterium proceeds mainly by single quasi-free proton-neutron scattering but that multiple scattering effects predominate in heavier nuclei.

PhysicsNuclear and High Energy PhysicsScatteringAstrophysics::High Energy Astrophysical PhenomenaNuclear Theorychemistry.chemical_elementPolarization (waves)Spectral lineNuclear physicsDeuteriumNeutron generatorchemistryAluminiumPhysics::Accelerator PhysicsNeutronAtomic physicsNuclear ExperimentNuclear Physics
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Double polarization experiments at intermediate energy

1999

At modern electron accelerators with highly polarized, intense, high duty factor beams double polarization coincidence experiments became feasible with good statistical accuracy. The strong potential towards the precise determination of small nucleon structure quantities is illustrated by two recent examples from MAMI. The measurement of $G_E^n$ in the quasifree reaction $D(\vec e, e'\vec n)p$ lead to a new parametrization of $G_E^n$ which is significantly above the previously preferred one from elastic $e-D$ scattering. A $p(\vec e, e'\vec p)\pi^0$ experiment at the energy of the $\Delta$ resonance yields preliminary results for the longitudinal quadrupole mixing. Both experimental errors …

PhysicsNuclear and High Energy PhysicsScatteringNuclear TheoryFOS: Physical sciencesElectronPolarization (waves)CoincidenceNuclear physicsIntermediate energyDuty cycleQuadrupoleNuclear Experiment (nucl-ex)NucleonNuclear ExperimentNuclear Experiment
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A Møller polarimeter for CW and pulsed intermediate energy electron beams

1990

The Moller polarimeter was mainly designed for the cw electron beam of the Mainz microtron (MAMI). The described polarimeter covers an energy range between 25 and 185 MeV and can relatively simply be upgraded to the maximum MAMI energy of 840 MeV. The Moller-scattered electrons are momentum-analyzed in the defocusing plane of a quadrupole magnet and both Moller electrons can be detected in coincidence for symmetrical scattering with ⊖cm=90°. All polarization components of the electron beam can be measured by suitable choices of the orientation of the target polarization. For pulsed electron beams with a small duty factor and a high peak current the polarimeter can also be operated with sing…

PhysicsNuclear and High Energy PhysicsScatteringbusiness.industryPolarimeterElectronPolarization (waves)OpticsPhysics::Atomic and Molecular ClustersCathode rayPhysics::Accelerator PhysicsRadial polarizationAtomic physicsNuclear ExperimentQuadrupole magnetbusinessInstrumentationMicrotronComputer Science::DatabasesNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Circinus X-1 observed with BeppoSAX wide field cameras

1999

Abstract We present a sky image and spectra for various orbital phases of Circinus X-1 observed by B-SAX Wide Field Cameras. We suggest that the spectral shape is dependent on the orbital phase.

PhysicsNuclear and High Energy PhysicsSpectral shape analysisAstrophysics::High Energy Astrophysical Phenomenamedia_common.quotation_subjectPhase (waves)AstronomyAstrophysicsWide fieldAtomic and Molecular Physics and OpticsSpectral lineSkyCircinusmedia_common
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Towards a new measurement of the neutron electric dipole moment

2009

International audience; The effort towards a new measurement of the neutron electric dipole moment (nEDM) at the Paul Scherrer Institut's (PSI) new high intensity source of ultracold neutrons (UCN) is described. The experimental technique relies on Ramsey's method of separated oscillatory fields, using UCN in vacuum with the apparatus at ambient temperature. In the first phase, R&D towards the upgrade of the RAL/Sussex/ILL apparatus is being performed at the Institut Laue-Langevin (ILL). In the second phase the apparatus, moved from ILL to PSI, will allow an improvement in experimental sensitivity by a factor of 5. In the third phase, a new spectrometer should gain another order of magnitud…

PhysicsNuclear and High Energy PhysicsTime reversal violationElectric dipole momentSpectrometerNeutron electric dipole momentPhysics::Instrumentation and Detectors010308 nuclear & particles physicsMagnetometerPhase (waves)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesMagnetic fieldlaw.inventionElectric dipole momentlawElectric field0103 physical sciencesUltracold neutronsAtomic physicsUltracold neutronsNuclear Experiment010306 general physicsInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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