Band termination in the N = Z odd-odd nucleus 46V -: art. no. 021303

被引：63
|
作者：
Lenzi, SM [1 ]
Napoli, DR
Ur, CA
Bazzacco, D
Brandolini, F
Cameron, JA
Caurier, E
de Angelis, G
De Poli, M
Farnea, E
Gadea, A
Hankonen, S
Lunardi, S
Martínez-Pinedo, G
Podolyak, Z
Poves, A
Alvarez, CR
Sánchez-Solano, J
Somacal, H
机构：
[1] Univ Padua, Dipartimento Fis, I-35131 Padua, Italy
[2] Ist Nazl Fis Nucl, Lab Nazl Legnaro, I-35020 Legnaro, Italy
[3] H Hulubei Natl Inst Phys & Nucl Engn, Bucharest, Romania
[4] McMaster Univ, Dept Phys & Astron, Hamilton, ON L8S 4M1, Canada
[5] Ctr Rech Nucl, F-67037 Strasbourg, France
[6] Univ Jyvaskyla, Dept Phys, FIN-40351 Jyvaskyla, Finland
[7] Aarhus Univ, DK-8000 Aarhus, Denmark
[8] Univ Autonoma Madrid, Dept Fis Teor C XI, E-28049 Madrid, Spain
来源：
PHYSICAL REVIEW C | 1999年 / 60卷 / 02期
关键词：
D O I：
10.1103/PhysRevC.60.021303
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：
High spin states in the odd-odd N = Z nucleus V-46 have been identified. At low spin, the T = 1 isobaric analog: states of Ti-46 are established up to I-pi = 6(+). Other high spin states, including the band terminating state, are tentatively assigned to the same T = 1 band. The T = 0 band built on the low-lying 3(+) isomer is observed up to the 1f(7/2)-shell termination at I-pi = 15(+). Both signatures of a negative parity T = 0 band are observed up to the terminating states at I-pi = 16(-) and I-pi = 17(-), respectively. The structure of this band is interpreted as a particle-hole excitation from the 1d(3/2) shell. Spherical shell model calculations are found to be in excellent agreement with the experimental results. [S0556-2813(99)50708-5].
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页数：5
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