Nuclear ground-state spins and magnetic moments of 27Mg, 29Mg, and 31Mg

被引:53
作者
Kowalska, M. [1 ]
Yordanov, D. T. [2 ]
Blaum, K. [1 ,3 ]
Himpe, P. [2 ]
Lievens, P. [4 ]
Mallion, S. [2 ]
Neugart, R. [1 ]
Neyens, G. [2 ]
Vermeulen, N. [2 ]
机构
[1] Johannes Gutenberg Univ Mainz, Inst Phys, D-55099 Mainz, Germany
[2] Katholieke Univ Leuven, Inst Kern & Stralingsfys, B-3001 Louvain, Belgium
[3] GSI Darmstadt, D-64291 Darmstadt, Germany
[4] Katholieke Univ Leuven, Vaste Stof Fys & Magnetisme Lab, B-3001 Louvain, Belgium
来源
PHYSICAL REVIEW C | 2008年 / 77卷 / 03期
关键词
D O I
10.1103/PhysRevC.77.034307
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The ground-state spins and magnetic moments of neutron-rich Mg-27, Mg-29, and Mg-31 were measured for the first time with laser and beta-NMR spectroscopy at ISOLDE/CERN. The hyperfine structure of Mg-27 observed in fluorescence-confirms previous assignments of the spin I = 1/2 and reveals the magnetic moment mu(I) (Mg-27) = -0.4107(15) mu(N). The hyperfine structure and nuclear magnetic resonance of optically polarized Mg-29-observed in the asymmetry of its beta decay after implantation in a cubic crystal-give I = 3/2 and mu(I) (Mg-29) = +0.9780(6) mu(N). For Mg-31 they yield together I = 1/2 and mu(I) (Mg-31) = -0.88355(15) mu(N), where the negative magnetic moment provides evidence for a positive parity. The results for 27Mg and 29Mg agree well with shell-model calculations confined only to the sd model space, whereas the ground state of Mg-31 involves large contributions from neutrons in the pf shell, which places this nucleus inside the "island of inversion.".
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页数:11
相关论文
共 51 条
[1]   BETA-DECAY OF NA-30 - EXPERIMENT AND THEORY [J].
BAUMANN, P ;
DESSAGNE, P ;
HUCK, A ;
KLOTZ, G ;
KNIPPER, A ;
MIEHE, C ;
RAMDANE, M ;
WALTER, G ;
MARGUIER, G ;
GABELMANN, H ;
RICHARDSERRE, C ;
SCHLOSSER, K ;
POVES, A .
PHYSICAL REVIEW C, 1989, 39 (02) :626-635
[2]   New "USD" Hamiltonians for the sd shell [J].
Brown, B. Alex ;
Richter, W. A. .
PHYSICAL REVIEW C, 2006, 74 (03)
[3]  
BROWN BA, 1988, ANNU REV NUCL PART S, V38, P29
[4]   The shell model as a unified view of nuclear structure [J].
Caurier, E ;
Martínez-Pinedo, G ;
Nowacki, F ;
Poves, A ;
Zuker, AP .
REVIEWS OF MODERN PHYSICS, 2005, 77 (02) :427-488
[5]   Large-scale shell model calculations for exotic nuclei [J].
Caurier, E ;
Nowacki, F ;
Poves, A .
EUROPEAN PHYSICAL JOURNAL A, 2002, 15 (1-2) :145-150
[6]  
Caurier E, 1999, ACTA PHYS POL B, V30, P705
[7]   Electric and nuclear transition strength in 30,32Mg [J].
Chisté, V ;
Gillibert, A ;
Lépine-Szily, A ;
Alamanos, N ;
Auger, F ;
Barrette, J ;
Braga, F ;
Cortina-Gil, MD ;
Dlouhy, Z ;
Lapoux, V ;
Lewitowicz, M ;
Lichtenthäler, R ;
Neto, RL ;
Lukyanov, SM ;
MacCormick, M ;
Marie, F ;
Mittig, W ;
Santos, FD ;
Orr, NA ;
Ostrowski, AN ;
Ottini, S ;
Pakou, A ;
Penionzhkevich, YE ;
Roussel-Chomaz, P ;
Sida, JL .
PHYSICS LETTERS B, 2001, 514 (3-4) :233-239
[8]   HARTREE-FOCK-BOGOLYUBOV CALCULATIONS WITH THE D-1 EFFECTIVE INTERACTION ON SPHERICAL NUCLEI [J].
DECHARGE, J ;
GOGNY, D .
PHYSICAL REVIEW C, 1980, 21 (04) :1568-1593
[9]  
DEMTRRODER W, 2003, LASER SPECTROSCOPY B, P34315
[10]   BETA-DECAY OF NA-27-32 AND THEIR DESCENDANTS [J].
DETRAZ, C ;
GUILLEMAUD, D ;
HUBER, G ;
KLAPISCH, R ;
LANGEVIN, M ;
NAULIN, F ;
THIBAULT, C ;
CARRAZ, LC ;
TOUCHARD, F .
PHYSICAL REVIEW C, 1979, 19 (01) :164-176