Search results for "Isotopes of tin"

showing 10 items of 23 documents

Absence of structure in the $^{20,22}$Ne + $^{118}$Sn quasi-elastic barrier distribution

2005

Abstract Motivated by the extreme deformation parameters of the projectile, we have measured quasi-elastic scattering for 20 Ne +  118 Sn. In contrast to calculations based on known collective states, the experimental barrier distribution is structureless. A comparison with the system 22 Ne +  118 Sn shows that this smoothing is unlikely to be due to nucleon- or α -transfer channels, and is more likely to be due to coupling to many other weak channels.

CouplingNuclear reactionPhysicsNuclear and High Energy PhysicsElastic Barrier010308 nuclear & particles physicsScattering22Ne[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCoupled channelsElectric fieldQuasi-elastic scattering0103 physical sciencesIsotopes of tin20Ne25.70.Bc; 25.70.Hi; 25.70.JjDeformation (engineering)Atomic physics010306 general physicsNucleonCoulomb barrier distribution
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Study of short-lived tin isotopes with a laser ion source

1995

A chemically selective laser ion source based on resonance ionization of atoms in a hot cavity has been applied for the study of short-lived silver isotopes at CERN/ ISOLDE. Silver atoms were ionized by two resonant excitations and final laser ionization into the continuum. Decay properties of the neutron-rich isotopes121–127Ag were studied with a neutron long-counter and aβ-detector.

Materials sciencePhysics::OpticsThermal ionizationLaserIon sourcelaw.inventionAtmospheric-pressure laser ionizationlawIonizationIsotopes of tinPhysics::Atomic and Molecular ClustersNeutronPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentAmbient ionizationAIP Conference Proceedings
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Optical spectroscopy using mass-separated beams: Nuclear properties of unstable indium and tin isotopes

1987

Abstract Collinear fast-beam laser-spectroscopy has been used to measure the hyperfine structure and isotope shift of several indium and tin isotopes. The related experimental techniques are described, including the preparation of mass-separated beams of neutron-deficient indium and tin isotopes at the GSI on-line mass separator following fusion-evaporation reactions. The deviation of the observed dependence of the charge radii upon the neutron number from the expected behaviour is briefly discussed.

Nuclear and High Energy PhysicsIsotopeRadiochemistrychemistry.chemical_elementCondensed Matter::Materials SciencechemistryNeutron numberIsotopes of tinPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentSpectroscopyInstrumentationHyperfine structureIndiumSeparator (electricity)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Systematics of Gamow-Teller beta decay “Southeast” of 100Sn

2010

The energy centroids and integrated strengths of Gamow-Teller transitions in the $ \beta^{+}_{}$ and electron-capture decay are analyzed for nuclei whose proton number Z and neutron number N are restricted to 44 $ \leq$ Z $ \leq$ 50 and 50 $ \leq$ N $ \leq$ 58 . The analysis is based on data measured both with high-resolution $ \gamma$ -ray spectrometry and total $ \gamma$ -ray absorption techniques. The dependence of the considered quantities on the relative neutron excess are established after taking into account the effects due to the Coulomb interaction and mean-field level occupancies. An extrapolation of this dependence to the lightest known tin isotopes is used to estimate the decay …

Nuclear physicsPhysicsNuclear and High Energy PhysicsProtonElectron captureNeutron numberIsotopes of tinHadronNuclear TheoryNeutronAbsorption (logic)Atomic numberAtomic physicsThe European Physical Journal A
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Production of Sn and Sb isotopes in high-energy neutron induced fission of natU

2018

The first systematic measurement of neutron-induced fission yields has been performed at the upgraded IGISOL-4 facility at the University of Jyväskylä, Finland. The fission products from high-energy neutron-induced fission of nat U were stopped in a gas cell filled with helium buffer gas, and were online separated with a dipole magnet. The isobars, with masses in the range A = 128-133 , were transported to a tape-implantation station and identified using γ -spectroscopy. We report here the relative cumulative isotopic yields of tin (Z = 50) and the relative independent isotopic yields of antimony (Z = 51). Isomeric yield ratios were also obtained for five nuclides. The yields of tin show a …

Nuclear reactionPhysicsNuclear and High Energy PhysicsFission products010308 nuclear & particles physicsFissionIsotopes of samariumFission product yield01 natural sciences7. Clean energyFast fissionNuclear physicsSubatomär fysikneutron-induced fission yields0103 physical sciencesIsotopes of tinSubatomic PhysicsNeutronsystematic measurement010306 general physics
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Laser Spectroscopy of Neutron-Rich Tin Isotopes: A Discontinuity in Charge Radii across the N=82 Shell Closure

2019

Physical review letters 122(19), 192502 (2019). doi:10.1103/PhysRevLett.122.192502

Physics MultidisciplinaryGeneral Physics and Astronomychemistry.chemical_elementLINE[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences530Effective nuclear chargeFORCECharge radiusDEPENDENCEMOMENTS0103 physical sciencesIsotopes of tinNeutronddc:530Nuclear Physics - Experiment010306 general physicsSpectroscopyNuclear ExperimentComputingMilieux_MISCELLANEOUSPhysicsScience & TechnologyNUCLEIPhysicsddc:chemistryPairingPhysical SciencesAtomic physicsTinNuclear density
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Mass measurements on unstable Sn and Sr isotopes with the ISOLTRAP mass spectrometer

2001

Direct mass measurements have been performed on the isotopes 76,77,80,81Sr and 129,130,131,132Sn by means of the Penning trap mass spectrometer ISOLTRAP at ISOLDE/CERN. In the case of 76Sr the mass was measured for the first time and an accuracy of about 30 keV was reached (Fig. 1). The masses of the tin isotopes are known for a long time from Q β measurements.

PhysicsLarge Hadron ColliderIsotope[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex][PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trapMass spectrometry01 natural sciencesISOLTRAP010305 fluids & plasmasNuclear physics0103 physical sciencesIsotopes of tin010306 general physics
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Nuclear symmetry energy and neutron skins derived from pygmy dipole resonances

2007

By exploiting Coulomb dissociation of high-energy radioactive beams of the neutron-rich nuclei $^{129\ensuremath{-}132}\mathrm{Sn}$ and $^{133,134}\mathrm{Sb}$, their dipole-strength distributions have been measured. A sizable fraction of ``pygmy'' dipole strength, energetically located below the giant dipole resonance, is observed in all of these nuclei. A comparison with available pygmy resonance data in stable nuclei ($^{208}\mathrm{Pb}$ and $N=82$ isotones) indicates a trend of strength increasing with the proton-to-neutron asymmetry. On theoretical grounds, employing the RQRPA approach, a one-to-one correlation is found between the pygmy strength and parameters describing the density d…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryHadronNuclear structureElementary particlereactions induced by unstable nucleiCoulomb excitation01 natural sciencesNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Dipole0103 physical sciencesIsotopes of tinNeutronAtomic physicsCoulomb excitation by heavy ionsNuclear Experiment010306 general physicsNucleonnuclear giant resonancesPhysical Review C
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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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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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