6533b872fe1ef96bd12d38b1
RESEARCH PRODUCT
g factors of $^{31,32,33}$Al: Indication for intruder configurations in the $^{33}$Al ground state
J. M. DaugasD. BorremansI. MateaS. MallionG. BélierK. T. FlanaganK. TurzóGerda NeyensN. SmirnovaN. VermeulenGeorgi P. GeorgievP. MorelD. L. BalabanskiM. De RydtDeyan YordanovYue PenionzhkevichP. HimpeC. StodelMagdalena KowalskaF. De Oliveira Santossubject
Nuclear reactionPhysicsNuclear and High Energy PhysicsMagnetic momentNUCLEISTABILITY010308 nuclear & particles physicsLandé g-factorMG-32[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesN=20 SHELL CLOSUREMODELMAGNETIC DIPOLEPhysics and AstronomyELECTRIC QUADRUPOLE-MOMENTS0103 physical sciencesSPECTROMETERAtomic physics010306 general physicsGround stateWave functionMagnetic dipoleSingle crystalDimensionless quantitydescription
Abstract The g factors of 31,32,33 Al have been measured using the β -nuclear magnetic resonance ( β -NMR) technique on spin-polarized beams produced in the fragmentation of a 36 S (77.5 MeV/u) beam on a 9 Be target. Nearly pure beams of Al ( Z = 13 ) isotopes were selected with the high-resolution fragment separator LISE at GANIL. An asymmetry as high as 6% has been observed in the β -NMR curve for 32 Al implanted in a Si single crystal. The magnetic moment of the N = 20 nucleus 33 Al is obtained for the first time: μ ( Al 33 , I π = 5 / 2 + ) = 4.088 ( 5 ) μ N , while those of 31,32 Al are obtained with improved accuracy: μ ( Al 31 , I π = 5 / 2 + ) = 3.830 ( 5 ) μ N and μ ( Al 32 , I π = 1 + ) = 1.9516 ( 22 ) μ N . Comparison of the results to shell-model calculations in the sd and the sdpf shell-model spaces leads to the conclusion that 33 Al must contain some contribution from 2 p – 2 h intruder configurations in its ground-state wave function. This indicates a gradual transition from the normal sd shell Si ( Z = 14 ) isotopes to the intruder Mg ( Z = 12 ) isotopes.
year | journal | country | edition | language |
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2006-12-01 |