γ-ray linear polarization measurements following heavy-ion bombardment of2s−1dshell nuclei

1975 ◽  
Vol 11 (1) ◽  
pp. 110-127 ◽  
Author(s):  
J. W. Olness ◽  
A. H. Lumpkin ◽  
J. J. Kolata ◽  
E. K. Warburton ◽  
J. S. Kim ◽  
...  
1975 ◽  
Vol 12 (2) ◽  
pp. 499-506 ◽  
Author(s):  
Jin Soon Kim ◽  
Y. K. Lee ◽  
K. A. Hardy ◽  
P. C. Simms ◽  
J. A. Grau ◽  
...  

2013 ◽  
Vol 87 (4) ◽  
Author(s):  
Y. Zheng ◽  
G. de France ◽  
E. Clément ◽  
A. Dijon ◽  
B. Cederwall ◽  
...  

1969 ◽  
Vol 19 (10) ◽  
pp. 1281-1289 ◽  
Author(s):  
J. Honzátko ◽  
J. Kajfosz

1967 ◽  
Vol 30 (4) ◽  
pp. 855 ◽  
Author(s):  
J. J. Butts ◽  
Robert Katz
Keyword(s):  

1970 ◽  
Vol 48 (7) ◽  
pp. 827-833 ◽  
Author(s):  
S. T. Lam ◽  
A. E. Litherland ◽  
J. J. Simpson

The 1459-keV level of 19F was populated by the 19F(p,p′γ)19F reaction at a proton energy of 2.78 MeV. The E2/M1 mixing ratio for the 1459 → 110 keV transition was determined to be [Formula: see text] from a combination of the γ-ray angular distribution and linear polarization and the nuclear lifetime. The γ-ray angular distribution was measured with a coaxial Ge(Li) detector and the γ-ray linear polarization with a planar Ge(Li) detector. The corresponding E2 and M1 transition strengths for a lifetime of 0.084 ± 0.020 ps are found to be [Formula: see text] and 0.10 ± 0.03 W.u. respectively. They are in good agreement with the particle–hole calculations of Benson and Flowers. The branching ratios of the 1459-keV level agree well with those of Poletti et al. The γ-ray transitions from the 1459-keV level provide a good example for demonstrating the usefulness of a single crystal Ge(Li) polarimeter.


1973 ◽  
Vol 7 (3) ◽  
pp. 1120-1132 ◽  
Author(s):  
E. K. Warburton ◽  
J. W. Olness ◽  
G. A. P. Engelbertink ◽  
T. K. Alexander

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