Gamow-Teller strength to K-38 from the Ar-38(p,n) reaction and Ca-38(beta(+)) decay

被引:24
作者
Anderson, BD
Baldwin, AR
Baumann, P
Brown, BA
Didierjean, F
Foster, CC
Garcia, LAC
Huck, A
Knipper, A
Madey, R
Manley, DM
Marguier, G
Ramdhane, M
Ravn, H
RichardSerre, C
Walter, G
Watson, JW
机构
[1] KENT STATE UNIV, NUCL RES CTR, KENT, OH 44242 USA
[2] UNIV STRASBOURG 1, CTR RECH NUCL, STRASBOURG, FRANCE
[3] MICHIGAN STATE UNIV, NATL SUPERCONDUCTING CYCLOTRON LAB, E LANSING, MI 48824 USA
[4] MICHIGAN STATE UNIV, DEPT PHYS, E LANSING, MI 48824 USA
[5] INDIANA UNIV, CYCLOTRON FACIL, BLOOMINGTON, IN 47408 USA
[6] HAMPTON UNIV, DEPT PHYS, HAMPTON, VA 23668 USA
[7] UNIV LYON 1, INST PHYS NUCL, F-69622 VILLEURBANNE, FRANCE
[8] CERN, ISOLDE COLLABORAT, CH-1211 GENEVA, SWITZERLAND
[9] IN2P3, GENEVA, SWITZERLAND
[10] UNIV CONSTANTINE, ECOLE NORMALE SUPER OUM EL BOUAGUI, CONSTANTINE, ALGERIA
来源
PHYSICAL REVIEW C | 1996年 / 54卷 / 02期
关键词
D O I
10.1103/PhysRevC.54.602
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
Gamow-Teller (1(+)) strength was studied in K-38 with the analog reactions Ar-38(p,n)K-38 and Ca-38(beta(+))K-38. The (p,n) reaction was performed at 135 MeV using the beam swinger facility at the Indiana University Cyclotron Facility. Excitation-energy spectra were measured at 15 angles between 0 degrees and 633. Neutron energies were measured by the time-of-flight method using a large-volume plastic scintillator array at a flight path of 131.0 m. The overall energy resolution was 280 keV. Gamow-Teller (GT) strength was extracted from the measured angular distributions to discrete 1(+) final states. The beta-decay experiment was performed with the ISOLDE on-line mass separator facility at CERN. The beta-decay branching ratios were determined by observing the delayed gamma decays of K-38. These decay measurements provide an increased sensitivity over earlier measurements and are able to extract transitions down to similar to 10(-4) of the strongest branches. The B(GT) values obtained from the two experiments are generally in good agreement, except for the transition to the first 1(+) state at 0.46 MeV, which is observed to be much weaker in the (p,n) measurements. The beta-decay measurements provide good resolution and high sensitivity while the (p,n) measurements extend the beta-decay measurements to higher excitation energies. The summed B(GT) strength is similar to 50% of the simple Ikeda sum rule. The distribution bf GT strength is in reasonable agreement with that predicted from a shell-model calculation using ''effective'' GT operators.
引用
收藏
页码:602 / 612
页数:11
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