Proton Capture Gamma Rays from the ReactionP31(p, γ)S32Leading to the Ground and First Excited States ofS32

1955 ◽  
Vol 99 (5) ◽  
pp. 1339-1344 ◽  
Author(s):  
E. B. Paul ◽  
H. E. Gove ◽  
A. E. Litherland ◽  
G. A. Bartholomew
1954 ◽  
Vol 94 (5) ◽  
pp. 1311-1316 ◽  
Author(s):  
R. R. Carlson ◽  
E. H. Geer ◽  
E. B. Nelson

1977 ◽  
Vol 285 (2) ◽  
pp. 189-197 ◽  
Author(s):  
K.A. Snover ◽  
P. Paul ◽  
H.M. Kuan

1989 ◽  
Vol 39 (2) ◽  
pp. 340-346 ◽  
Author(s):  
J. D. Kalen ◽  
H. J. Hausman ◽  
A. Abduljalil ◽  
W. Kim ◽  
D. G. Marchlenski ◽  
...  

1973 ◽  
Vol 51 (7) ◽  
pp. 707-712 ◽  
Author(s):  
P. G. Kerr ◽  
A. W. Gibb ◽  
J. A. Cameron

The (α,n) reaction on natural chromium has been used to study levels in 55Fe up to 2.5 MeV excitation. Intensities and angular distributions of the decay gamma rays were measured, yielding branching and E2/M1 mixing ratios. In a magnetized target of the alloy Cr20Fe80, the rotation of the angular distributions was observed. Using recently determined lifetimes for the excited states and the average internal field of 277 kOe measured in the target material by Mössbauer absorption, the following g factors are obtained:[Formula: see text]


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

1970 ◽  
Vol 152 (2) ◽  
pp. 257-262 ◽  
Author(s):  
A.R. Barnett ◽  
N.W. Tanner

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.


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