The structure of S-32 .2. Shell model interpretation

被引:11
作者
Brenneisen, J [1 ]
Erhardt, B [1 ]
Glatz, F [1 ]
Kern, T [1 ]
Ott, R [1 ]
Ropke, H [1 ]
Schmalzlin, J [1 ]
Siedle, P [1 ]
Wildenthal, BH [1 ]
机构
[1] UNIV TEXAS,SCH NAT SCI & MATH,PHYS PROGRAM,RICHARDSON,TX 75083
来源
ZEITSCHRIFT FUR PHYSIK A-HADRONS AND NUCLEI | 1997年 / 357卷 / 04期
关键词
D O I
10.1007/s002180050257
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 properties of positive-parity states in S-32 are compared to predictions of shell. model calculations within the complete s-d basis space using the universal s-d shell Hamiltonian. The experimental T = O spectrum is reproduced to excitation energies between 10 and 11.7 MeV, depending on the level spins. The T = 1 spectrum is known and reproduced for the first five 5 MeV in excitation in general and for the first 8 MeV in the case of I-pi = 1(+) states. Altogether the excitation energies of 80 positive-parity states are reproduced with a rms deviation of 200 keV. A calculation of radiative widths and branching ratios for gamma-decay which uses effective charges and free-nucleon g-factors yields good general agreement with experiment. The need for effective g-factors is felt only in the rare cases of transitions which are governed by the isovector d(3/2) --> d(5/2) M1 matrix element. The spectrum of negative parity, T = 1 states is understood in terms of the weakcoupling model while that of the T = 0 states is comprised of octupole-quadrupole phonon multiplets. Positive-parity states from outside the s-d configuration are first observed between 9.5 and 10.5 MeV excitation energy.
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页码:377 / 386
页数:10
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