Search results for "Hyperfine structure"

showing 10 items of 423 documents

Nuclear moments and charge radii of bismuth isotopes

2000

Isotope shifts and hyperfine structures have been measured on the 306.7 nm line in bismuth isotopes with A = 205-210, 210m, 212 and 213 by gas cell laser spectroscopy. More precise measurements were made for the A = 207-209 isotopes in atomic beam measurements. Nuclear magnetic and quadrupole moments were deduced. A detailed comparison of the nuclear charge radii systematics has been made in the region using a King plot technique.

PhysicsNuclear and High Energy PhysicsIsotopechemistry.chemical_elementEffective nuclear chargeBismuthchemistryQuadrupolePhysics::Atomic PhysicsAtomic physicsNuclear ExperimentAtomic vapor laser isotope separationSpectroscopyHyperfine structureLine (formation)Journal of Physics G: Nuclear and Particle Physics
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Atomic beam magnetic resonance apparatus for systematic measurement of hyperfine structure anomalies (Bohr-Weisskopf effect)

1993

Abstract An atomic beam magnetic resonance (ABMR) apparatus has been constructed at Orsay, and has been installed at the CERN PS Booster ISOLDE mass separator facility for “on-line” work with radioactive isotopes in a program to measure hyperfine structure anomalies (the Bohr-Weisskopf effect) over long isotopic chains. The hfs anomalies result from the effect of the spatial distribution of the nuclear magnetization on the atomic hfs interaction. Constructional details of the system are described: emphasis is placed on the measurement of nuclear g-factors by a triple resonance, laser state selected, ABMR method. A precision better than 10−4 for gI values has been obtained in stable atomic b…

PhysicsNuclear and High Energy PhysicsIsotopechemistry.chemical_elementThermal ionizationMass spectrometryLaserlaw.inventionBohr modelNuclear physicsMagnetizationsymbols.namesakechemistrylawCaesiumsymbolsPhysics::Accelerator PhysicsPhysics::Atomic PhysicsDetectors and Experimental TechniquesAtomic physicsNuclear ExperimentInstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Das Vorzeichen der Hyperfeinstruktur-Aufspaltung des 3d 5 4s 2 6 S 5/2-Grundzustandes des Mn55

1962

Using a double Fabry-Perot interferometer and an atomic-beam light source, the sign of the hyperfine-structure splitting of the 3d 5 4s 2 6 S 5/2 ground state of Mn55 has been determined to be negative. The absolute value of the splitting previously has been measured byWoodgate andMartin.

PhysicsNuclear and High Energy PhysicsLight sourceAbsolute valueAtomic physicsGround stateHyperfine structureSign (mathematics)Zeitschrift für Physik
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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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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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Spin, moments, and mean square nuclear charge radius ofSr77

1992

The neutron deficient $^{77}\mathrm{Sr}$ nucleus was studied by fast ion beam collinear laser spectroscopy with a detection scheme based on optical pumping, state selective neutralization, and atom counting. From the measured hyperfine splitting and isotope shift of the Sr II transition 5s $^{2}$${\mathit{S}}_{1/2}$\ensuremath{\rightarrow}5p $^{2}$${\mathit{P}}_{3/2}$ the nuclear spin I=5/2, the nuclear moments \ensuremath{\mu}=-0.348(4)${\mathrm{\ensuremath{\mu}}}_{\mathit{N}}$, ${\mathit{Q}}_{\mathit{s}}$=1.40(11) b, and the change in mean square charge radius \ensuremath{\delta}〈${\mathit{r}}^{2}$${\mathrm{〉}}^{88,77}$=0.248(12) ${\mathrm{fm}}^{2}$ were deduced. These ground-state proper…

PhysicsNuclear and High Energy PhysicsMagnetic momentCharge radiusAtomCharge densityAtomic physicsGround stateSpin (physics)Hyperfine structureEffective nuclear chargePhysical Review C
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Nuclear ground-state spins and magnetic moments ofMg27,Mg29, andMg31

2008

The ground-state spins and magnetic moments of neutron-rich {sup 27}Mg, {sup 29}Mg, and {sup 31}Mg were measured for the first time with laser and {beta}-NMR spectroscopy at ISOLDE/CERN. The hyperfine structure of {sup 27}Mg--observed in fluorescence--confirms previous assignments of the spin I=1/2 and reveals the magnetic moment {mu}{sub I}({sup 27}Mg)=-0.4107(15){mu}{sub N}. The hyperfine structure and nuclear magnetic resonance of optically polarized {sup 29}Mg--observed in the asymmetry of its {beta} decay after implantation in a cubic crystal--give I=3/2 and {mu}{sub I}({sup 29}Mg)=+0.9780(6){mu}{sub N}. For {sup 31}Mg they yield together I=1/2 and {mu}{sub I}({sup 31}Mg)=-0.88355(15){…

PhysicsNuclear and High Energy PhysicsMagnetic momentIsland of inversionHadronAtomic physicsNucleonGround stateIsotopes of magnesiumHyperfine structureRadioactive decayPhysical Review C
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Systematic measurements of the bohr-weisskpf effect at isolde

1992

The hyperfine anomaly gives an insight into the coupling of spin and orbital magnetic moments in the nucleus. More precisely, the nuclear magnetization is expressible through the nuclear wave functions with which is tested not only the magnetic moment operator, but also the tensor product [s×C2]1. The experiment can then be expected to be of value in testing the nuclear structure theory. The greatest value of these measurements is gained when these are made systematically over a large number of isotopes. We propose to initiate a program at ISOLDE to measure the hyperfine anomaly systematically in the heavy alkali elements. The experimental setup to achieve, in particular, a precise measurem…

PhysicsNuclear and High Energy PhysicsMagnetic momentNuclear structureCondensed Matter PhysicsAtomic and Molecular Physics and OpticsBohr modelNuclear physicsMagnetizationsymbols.namesakeNuclear magnetic momentsymbolsPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsAnomaly (physics)Nuclear ExperimentSpin (physics)Hyperfine structureHyperfine Interactions
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Shell structure of potassium isotopes deduced from their magnetic moments

2014

\item[Background] Ground-state spins and magnetic moments are sensitive to the nuclear wave function, thus they are powerful probes to study the nuclear structure of isotopes far from stability. \item[Purpose] Extend our knowledge about the evolution of the $1/2^+$ and $3/2^+$ states for K isotopes beyond the $N = 28$ shell gap. \item[Method] High-resolution collinear laser spectroscopy on bunched atomic beams. \item[Results] From measured hyperfine structure spectra of K isotopes, nuclear spins and magnetic moments of the ground states were obtained for isotopes from $N = 19$ up to $N = 32$. In order to draw conclusions about the composition of the wave functions and the occupation of the …

PhysicsNuclear and High Energy PhysicsMagnetic momentProtonNuclear Theory010308 nuclear & particles physicsNuclear structureFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energy3. Good healthNuclear Theory (nucl-th)Atomic orbitalIsotopes of potassium0103 physical sciencesNeutronNuclear Physics - ExperimentAtomic physicsPräzisionsexperimente - Abteilung BlaumNuclear Experiment (nucl-ex)010306 general physicsGround stateHyperfine structureNuclear Experiment
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Laser-microwave spectroscopy of the hyperfine structure of 9Be for the investigation of unstable Be isotopes

1997

Abstract For an investigation concerning the nuclear magnetic moments and their distributions in the nuclei of 7,11Be, an experimental project using laser-microwave double resonance spectroscopy for trapped ions is under progress at INS. Laser cooled ion crystals consisting of a few 9Be+ ions were observed and the ground state hyperfine splitting of 9Be+ was measured with a precision of 10−5. Experiments on the unstable isotope 7Be have been started.

PhysicsNuclear and High Energy PhysicsMagnetic momentResonanceLaserIonlaw.inventionlawPhysics::Atomic PhysicsRotational spectroscopyAtomic physicsGround stateSpectroscopyHyperfine structureNuclear PhysicsNuclear Physics A
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