CONSTRAINTS ON THE LOW-ENERGY E1 CROSS-SECTION OF C-12(ALPHA,GAMMA-O-16 FROM THE BETA-DELAYED ALPHA-SPECTRUM OF N-16

被引:162
|
作者
AZUMA, RE
BUCHMANN, L
BARKER, FC
BARNES, CA
DAURIA, JM
DOMBSKY, M
GIESEN, U
JACKSON, KP
KING, JD
KORTELING, RG
MCNEELY, P
POWELL, J
ROY, G
VINCENT, J
WANG, TR
WONG, SSM
WREAN, PR
机构
[1] TRIUMF, VANCOUVER V6T 2A3, BC, CANADA
[2] AUSTRALIAN NATL UNIV, RES SCH PHYS SCI & ENGN, DEPT THEORET PHYS, CANBERRA, ACT 0200, AUSTRALIA
[3] CALTECH, WK KELLOGG LAB, PASADENA, CA 91125 USA
[4] SIMON FRASER UNIV, DEPT CHEM, BURNABY V5A 1S6, BC, CANADA
[5] UNIV ALBERTA, DEPT PHYS, EDMONTON T6G 2J1, ALBERTA, CANADA
来源
PHYSICAL REVIEW C | 1994年 / 50卷 / 02期
关键词
D O I
10.1103/PhysRevC.50.1194
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 shape of the low-energy part of the beta-delayed alpha-particle spectrum of N-16 is very sensitive to the alpha+C-12 reduced width of the 7.117 MeV subthreshold state of O-16. This state, in turn, dominates the low-energy p-wave capture amplitude of the astrophysically important C-12(alpha, gamma)O-16 reaction. The alpha spectrum following the decay of N-16 has been measured by producing a low-energy (NN+)-N-16-N-14 beam with the TRIUMF isotope separator TISOL, stopping the molecular ions in a foil, and counting the alpha particles and C-12 recoil nuclei in coincidence, in thin surface-barrier detectors. In addition to obtaining the alpha spectrum, this procedure determines the complete detector response including the low-energy tail. The spectrum, which contains more than 10(6) events, has been fitted by R- and K-matrix parametrizations which include the measured C-12(alpha, gamma)O-16 cross section and the measured alpha+C-12 elastic-scattering phase shifts. The model space appropriate for these parametrizations has been investigated. For S(E1)(300), the E1 part of the astrophysical S factor for the C-12(alpha, gamma)O-16 reaction at E(c.m.) = 300 keV, values of 79 +/- 21 and 82 +/- 26 keV b have been derived from the R- and K-matrix fits, respectively.
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页码:1194 / 1215
页数:22
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