0000000000281439

AUTHOR

J. Sauvage

showing 6 related works from this author

Large Odd-even Radius Staggering In The Very Light Platinum Isotopes From Laser Spectroscopy

1999

Laser spectroscopy measurements have been carried out on very-neutron-deficient platinum isotopes with the COMPLIS experimental setup. Using the ${5d}^{9}{6s}^{3}{D}_{3}\ensuremath{\rightarrow}{5d}^{9}{6p}^{3}{P}_{2}$ optical transition, hyperfine spectra of ${}^{182,181,180,179,178}\mathrm{Pt}$ and ${}^{183}{\mathrm{Pt}}^{m}$ were recorded for the first time. The variation of the mean square charge radius between these nuclei, the magnetic moments of the odd isotopes, and the quadrupole moment of ${}^{183}{\mathrm{Pt}}^{m}$ were thus measured. A large deformation change between ${}^{183}{\mathrm{Pt}}^{g}$ and ${}^{183}{\mathrm{Pt}}^{m},$ an odd-even staggering of the charge radius, and a d…

PhysicsNuclear and High Energy PhysicsMagnetic moment010308 nuclear & particles physicsNuclear Theorychemistry.chemical_elementCharge density[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]XX7. Clean energy01 natural sciencesSpectral linechemistryCharge radius0103 physical sciencesQuadrupoleAtomic physics010306 general physicsSpectroscopyPlatinumHyperfine structure
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Yields of neutron-rich rubidium and cesium isotopes from fast-neutron induced fission of 238U, obtained by studying their release from a thick ISOL t…

2006

Abstract In the framework of the EURISOL project, the production of neutron-rich isotopes of rubidium and cesium has been studied. The intensities of mass-separated beams of rubidium and cesium isotopes generated from a thick 238 UC x target connected to a surface ionizer have been measured. The release properties of 140 Cs and 91 Rb have been investigated. The obtained results allowed us to determine the relative fission yields of rubidium and cesium isotopes with high accuracy.

Nuclear and High Energy PhysicsCesium IsotopeschemistryIsotopeFissionCaesiumRadiochemistrychemistry.chemical_elementNeutronInstrumentationIsotopes of caesiumRubidiumNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Charge radius changes of even-even neutron-rich Tellurium isotopes

2005

Laser spectroscopy based on resonant ionization of laser-desorbed atoms has been used to study the neutron-rich tellurium isotopes with the COMPLIS facility at ISOLDE-CERN. The isotope shift and the hyperfine structure of several neutron-rich Te isotopes: $^{120–136}$Te and $^{123m–133m}$Te have been measured. From the hyperfine structure and the isotope shift we can extract the magnetic and quadrupole moments and the change in the mean square charge radius respectively. The mean square charge radii of the even-even isotopes have been deduced and their comparison with the known data for the other elements near Z=50 is presented. The experimental $\delta$ is compared with that obtained from …

spectroscopyIsotope27.60.+j 29.30.-h010308 nuclear & particles physicsChemistryNuclear structure[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyCharge radiusIonizationtellurium0103 physical sciencesQuadrupolenuclear structureNuclei with mass number 90 to 149NeutronPhysics::Atomic Physicslaser beam applicationsAtomic physics010306 general physicsSpectroscopyNuclear ExperimentHyperfine structure
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Charge-radius change and nuclear moments in the heavy tin isotopes from laser spectroscopy: Charge radius ofSn132

2005

Laser spectroscopy measurements have been carried out on the neutron-rich tin isotopes with the COMPLIS experimental setup. Using the $5{s}^{2}5{p}^{2\phantom{\rule{0.3em}{0ex}}3}{P}_{0}\ensuremath{\rightarrow}5{s}^{2}5p6s\phantom{\rule{0.3em}{0ex}}{}^{3}{P}_{1}$ optical transition, hyperfine spectra of $^{126\ensuremath{-}132}\mathrm{Sn}$ and $^{125,127,129\ensuremath{-}131}\mathrm{Sn}{}^{m}$ were recorded for the first time. The nuclear moments and the mean square charge radius variation ($\ensuremath{\delta}\ensuremath{\langle}{r}_{c}^{2}\ensuremath{\rangle}$) were extracted. From the quadrupole moment values, these nuclei appear to be spherical. The magnetic moments measured are thus co…

PhysicsNuclear and High Energy PhysicsMagnetic moment010308 nuclear & particles physicsCharge density7. Clean energy01 natural sciencesSpectral lineMean field theoryCharge radius0103 physical sciencesQuadrupoleIsotopes of tinAtomic physics010306 general physicsHyperfine structurePhysical Review C
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Nuclear Moments and Deformation Change inA184ug,mfrom Laser Spectroscopy

1997

Resonance ionization spectroscopy (RIS) was performed on desorbed Au, and the complete hyperfine spectrum of both isomeric and ground states of the short lived 184Au nucleus has been recorded from the 5d106s S1y2 ! 5d106p P3y2 optical transition. The nuclear moments of both states and the mean square charge radius changes were measured. The magnetic moments were determined to be m 184g I­5 ­ 12.07s2dmN and m I­2 ­ 11.44s2dmN and the spectroscopic quadrupole moments to be Q 184g s ­ 14.65s26db and Q184m s ­ 11.90s16d b. A difference in the mean square charge radius dkr2 c l184g,184m ­ 20.036s3d fm2 was found. [S0031-9007(97)03992-6]

PhysicsMagnetic momentCharge radiusOptical transitionQuadrupoleResonance ionizationGeneral Physics and AstronomyDeformation (engineering)Atomic physicsSpectroscopyHyperfine structurePhysical Review Letters
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Charge radius change in the heavy tin isotopes until A = 132 from laser spectroscopy

2001

Laser spectroscopy measurements have been carried out on the very neutron-rich tin isotopes with the COMPLIS experimental setup. Using the 5s 25p 23P 0 → 5s 25p6s 3P 1 optical transition, hyperfine spectra of 126-132Sn and 125m, 127m, 129m-131mSn where recorded for the first time. The variation of the mean-square charge radius ( δ〈r 2〉) between these nuclei and nuclear moments of the isomers and the odd isotopes were thus measured. An odd-even staggering which inverts at A = 130 is clearly observed. This indicates a small appearance of a plateau on the δ〈r 2〉 which has to be confirmed by measuring the isotope shift beyond A = 132.

PhysicsNuclear and High Energy PhysicsIsotopeChemistry010308 nuclear & particles physicsJahn–Teller effect[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Plateau (mathematics)01 natural sciencesSpectral lineCharge radius0103 physical sciencesIsotopes of tinNuclear fusionAtomic physics010306 general physicsSpectroscopyHyperfine structure
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