scholarly journals PROTON CAPTURE GAMMA RAYS FROM Si$sup 28$ IN THE REGION OF THE PHOTONUCLEAR GIANT RESONANCE (thesis)

1961 ◽  
Author(s):  
C.C. Gardner
1959 ◽  
Vol 3 (4) ◽  
pp. 177-179 ◽  
Author(s):  
H. E. Gove ◽  
A. E. Litherland ◽  
R. Batchelor

1961 ◽  
Vol 26 (3) ◽  
pp. 480-510 ◽  
Author(s):  
H.E. Gove ◽  
A.E. Litherland ◽  
R. Batchelor

1967 ◽  
Vol 157 (4) ◽  
pp. 921-928 ◽  
Author(s):  
L. Feldman ◽  
B. B. Baliga ◽  
M. Nessin

1954 ◽  
Vol 94 (5) ◽  
pp. 1311-1316 ◽  
Author(s):  
R. R. Carlson ◽  
E. H. Geer ◽  
E. B. Nelson

1983 ◽  
Vol 399 (1) ◽  
pp. 66-82 ◽  
Author(s):  
M. Anghinolfi ◽  
P. Corvisiero ◽  
G. Ricco ◽  
M. Taiuti ◽  
A. Zucchiatti

1962 ◽  
Vol 15 (3) ◽  
pp. 443 ◽  
Author(s):  
AW Parker ◽  
GG Shute

From a recent experiment in this laboratory (Shute et al. 1962) on the elastic scattering of protons from 12C, resonance levels (E13N, J1t) of 13N were obtained at the laboratory bombarding energies (Ep) shown in Table 1. To confirm these results, an investigation of the yield and angular distribution of gamma rays from the reaction 12C(p'YO)13N and 12C(p'Yl)13N was undertaken. Accordingly, the theoretical angular distributions, W(8), for the gamma ray (Yo) to the ground state of 13Na-) and also for the gamma ray (Yl) to the 1st excited state of 13Na+) were evaluated on the assumptions that overlap of levels in 13N is small and lowest order multipoles are involved. As angular distributions are parity insensitive, these were found to be identical for the two gamma rays expected. The simpler of these angular distributions are also shown on the table. The expected angular distributions indicate that 90� is a suitable angle for yield curves.


1960 ◽  
Vol 4 (2) ◽  
pp. 92-92 ◽  
Author(s):  
S. G. Cohen ◽  
P. S. Fisher ◽  
E. K. Warburton
Keyword(s):  

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