0000000000205268

AUTHOR

F. D. Smit

showing 7 related works from this author

Complete Electric Dipole Response and the Neutron Skin inPb208

2011

A benchmark experiment on Pb-208 shows that polarized proton inelastic scattering at very forward angles including 0 degrees is a powerful tool for high-resolution studies of electric dipole (E1) and spin magnetic dipole (M1) modes in nuclei over a broad excitation energy range to test up-to-date nuclear models. The extracted E1 polarizability leads to a neutron skin thickness r(skin) = 0.156(-0.021)(+0.025) fm in Pb-208 derived within a mean-field model [Phys. Rev. C 81, 051303 (2010)], thereby constraining the symmetry energy and its density dependence relevant to the description of neutron stars.

PhysicsDipoleProtonPolarizabilityGeneral Physics and AstronomyNeutronInelastic scatteringElectric dipole transitionAtomic physicsMagnetic dipoleExcitationPhysical Review Letters
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Pygmy dipole resonance in208Pb

2012

Scattering of protons of several hundred MeV is a promising new spectroscopic tool for the study of electric dipole strength in nuclei. A case study of 208Pb shows that at very forward angles J^pi = 1- states are strongly populated via Coulomb excitation. A separation from nuclear excitation of other modes is achieved by a multipole decomposition analysis of the experimental cross sections based on theoretical angular distributions calculated within the quasiparticle-phonon model. The B(E1) transition strength distribution is extracted for excitation energies up to 9 MeV, i.e., in the region of the so-called pygmy dipole resonance (PDR). The Coulomb-nuclear interference shows sensitivity to…

PhysicsNuclear and High Energy PhysicsNuclear TheoryScatteringTransition dipole momentFOS: Physical sciencesCoulomb excitationResonance (particle physics)Nuclear Theory (nucl-th)DipoleNuclear Experiment (nucl-ex)Atomic physicsElectric dipole transitionNuclear ExperimentMultipole expansionNuclear ExperimentExcitationPhysical Review C
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Complete dipole response in [sup 208]Pb from high-resolution polarized proton scattering at 0°

2009

At the Research Center for Nuclear Physics, Osaka, Japan, the 208Pb(p,p´) reaction was measured at Ep=295 MeV and scattering angles Θlab= 0° - 10°. A high energy resolution of the order of ΔE/E ≈ 8x10^-5 was achieved, corresponding to ΔE=25-30 keV (FWHM). Cross sections were extracted by a multipole decomposition analysis of the angular distributions. Dominant contributions at very forward angles originate from E1 excitation due to Coulomb projectile-target interaction and spin M1 transitions caused by the spin-isospin part of the proton-nucleus interaction. A separation of these contributions was performed with two independent methods, viz. a multipole decomposition of the angular distribu…

PhysicsDipolePolarizabilityScatteringNeutronAtomic physicsFermi gasMultipole expansionSpin (physics)Resonance (particle physics)AIP Conference Proceedings
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A study of fusion - fission atZ= 107

1997

An experiment was performed with the EUROGAM II array to investigate the reaction channels that are open in the fusion of a beam on the actinide target at a series of energies around the Coulomb barrier. The symmetric fission products identified from the level structures seem to suggest that a proton and neutrons are emitted prior to fission.

Nuclear physicsPhysicsNuclear and High Energy PhysicsFission productsCold fissionCluster decayNeutron emissionFissionNuclear TheoryFission product yieldNuclear ExperimentDelayed neutronFast fissionJournal of Physics G: Nuclear and Particle Physics
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Study of M1 and E1 excitations by high-resolution proton inelastic scattering measurement at forward angles

2007

Experimental technique for measuring proton inelastic scattering with high‐resolution at 295 MeV and at forward angles including zero degrees is described. The method is useful for extracting spin part of the M1 strength via nuclear excitation as well as E1 strength via Coulomb excitation. An excitation energy resolution of 20 keV, good scattering angle resolution, and low background condition have been achieved. The experimental technique was applied for several sd and pf shell nuclei.

PhysicsProtonScatteringNuclear TheoryResolution (electron density)Coulomb excitationProton emissionMott scatteringInelastic scatteringAtomic physicsExcitationAIP Conference Proceedings
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Nonquenched Isoscalar Spin-M1Excitations insd-Shell Nuclei

2015

Differential cross sections of isoscalar and isovector spin-M1 (0(+)→1(+)) transitions are measured using high-energy-resolution proton inelastic scattering at E(p)=295  MeV on (24)Mg, (28)Si, (32)S, and (36)Ar at 0°-14°. The squared spin-M1 nuclear transition matrix elements are deduced from the measured differential cross sections by applying empirically determined unit cross sections based on the assumption of isospin symmetry. The ratios of the squared nuclear matrix elements accumulated up to E(x)=16  MeV compared to a shell-model prediction are 1.01(9) for isoscalar and 0.61(6) for isovector spin-M1 transitions, respectively. Thus, no quenching is observed for isoscalar spin-M1 transi…

PhysicsMatrix (mathematics)IsovectorProtonIsospinIsoscalarNuclear TheoryStochastic matrixGeneral Physics and AstronomyInelastic scatteringAtomic physicsNuclear ExperimentSpin (physics)Physical Review Letters
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Measurement of high energy resolution inelastic proton scattering at and close to zero degrees

2009

13 pages, 15 figures.-- Printed version published Jul 1, 2009.

Nuclear and High Energy PhysicsHigh energy resolutionM1 excitationForward scatterCyclotronMeasurement at 0 degreesTRANSITIONSInelastic scatteringDispersion matchingISOVECTORlaw.inventionSHELL NUCLEINuclear physicsNUCLEON-NUCLEON INTERACTIONlawBEAM LINEE1 Coulomb excitationFOCAL-PLANE POLARIMETERInstrumentationInelastic proton scatteringPolarization transfer coefficientsISOSCALARElastic scatteringPhysicsBackground subtractionPolarization transfer coefficientScatteringResolution (electron density)SPIN EXCITATIONSBeamlinePhysics::Accelerator PhysicsMeasurement at 0ºAtomic physicsSPECTROMETER GRAND RAIDENINTERMEDIATE ENERGIES
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