Search results for "N=28"

showing 2 items of 2 documents

Changes in nuclear structure along the Mn isotopic chain studied via charge radii

2016

The hyperfine spectra of $^{51,53-64}$Mn were measured in two experimental runs using collinear laser spectroscopy at ISOLDE, CERN. Laser spectroscopy was performed on the atomic $3d^5\ 4s^2\ ^{6}\text{S}_{5/2}\rightarrow 3d^5\ 4s4p\ ^{6}\text{P}_{3/2}$ and ionic $3d^5\ 4s\ ^{5}\text{S}_2 \rightarrow 3d^5\ 4p\ ^{5}\text{P}_3$ transitions, yielding two sets of isotope shifts. The mass and field shift factors for both transitions have been calculated in the multiconfiguration Dirac-Fock framework and were combined with a King plot analysis in order to obtain a consistent set of mean-square charge radii which, together with earlier work on neutron-deficient Mn, allow the study of nuclear struc…

Nuclear and High Energy PhysicsField (physics)N=28FOS: Physical sciences114 Physical sciences01 natural sciencesSpectral line0103 physical sciencesPROGRAMNuclear Physics - ExperimentNeutronNuclear Experiment (nucl-ex)LASER SPECTROSCOPY010306 general physicsSpectroscopyCALCIUM ISOTOPESNuclear ExperimentHyperfine structureisotopesPhysicsisotoopitta114010308 nuclear & particles physicsNuclear structureSHIFTShyperfine spectraOrder (ring theory)Charge (physics)mangaaniQUADRUPOLE-MOMENTSnuclear structuremanganeseSHELL-MODELlaser spectroscopyNEUTRONPräzisionsexperimente - Abteilung BlaumAtomic physicsPhysical Review C
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Magnetic and quadrupole moments of neutron deficient 58-62Cu isotopes

2011

Abstract This paper reports on the ground state nuclear moments measured in 58–62Cu using collinear laser spectroscopy at the ISOLDE facility. The quadrupole moments for 58–60Cu have been measured for the first time as Q ( Cu 58 ) = − 15 ( 3 ) efm 2 , Q ( Cu 59 ) = − 19.3 ( 19 ) efm 2 , Q ( Cu 60 ) = + 11.6 ( 12 ) efm 2 and with higher precision for 61,62Cu as Q ( Cu 61 ) = − 21.1 ( 10 ) efm 2 , Q ( Cu 62 ) = − 2.2 ( 4 ) efm 2 . The magnetic moments of 58,59Cu are measured with a higher precision as μ ( Cu 58 ) = + 0.570 ( 2 ) μ N and μ ( Cu 59 ) = + 1.8910 ( 9 ) μ N . The experimental nuclear moments are compared to large-scale shell-model calculations with the GXPF1 and GXPF1A effective i…

PhysicsNuclear and High Energy Physicsnuclear-structureIsotopeMagnetic momentNuclear moments010308 nuclear & particles physicsshell-modelNuclear structureN=287. Clean energy01 natural sciencesShell modelCu58Cu59Cu60Cu61Cu620103 physical sciencesQuadrupoleNuclear spinNeutronHyperfine structureAtomic physicsLaser spectroscopy010306 general physicsGround stateSpectroscopyHyperfine structure
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