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Determination of theE1component of the low-energyC12(α,γ)O16cross section

Authors :
K. E. Rehm
M. Paul
J. P. Schiffer
R. C. Pardo
D. Kahl
Guy Savard
X. D. Tang
I. Ahmad
Masahiro Notani
S. K. Sinha
A. H. Wuosmaa
Arthur E Champagne
R. E. Segel
John P. Greene
D. J. Henderson
E. F. Moore
R. V. F. Janssens
A. A. Hecht
C. L. Jiang
L. Jisonna
N. Patel
Carl R. Brune
Source :
Physical Review C. 81
Publication Year :
2010
Publisher :
American Physical Society (APS), 2010.

Abstract

A measurement of the $\ensuremath{\beta}$-delayed $\ensuremath{\alpha}$ decay of $^{16}\mathrm{N}$ using a set of twin ionization chambers is described. Sources were made by implantation, using a $^{16}\mathrm{N}$ beam produced via the In-Flight Technique. The energies and emission angles of the $^{12}\mathrm{C}$ and $\ensuremath{\alpha}$ particles were measured in coincidence and very clean $\ensuremath{\alpha}$ spectra, down to energies of $450$ keV, were obtained. The structure of the spectra from this experiment is in good agreement with results from previous measurements. An analysis of our data with the same input parameters as used in earlier studies gives ${S}_{E1}(300)=86\ifmmode\pm\else\textpm\fi{}22$ keVb for the $E1$ component of the $S$-factor. This value is in excellent agreement with results obtained from various direct and indirect measurements. In addition, the influence of new measurements including the phase shift data from Tischhauser et al. on the value of ${S}_{E1}(300)$ is discussed.

Details

ISSN :
1089490X and 05562813
Volume :
81
Database :
OpenAIRE
Journal :
Physical Review C
Accession number :
edsair.doi...........824076d511fd962910d71787b42ec196
Full Text :
https://doi.org/10.1103/physrevc.81.045809