Absolute Intensities of Resonance Neutron Capture Gamma Rays from Cd, Te, and Sm

1957 ◽  
Vol 107 (6) ◽  
pp. 1650-1654 ◽  
Author(s):  
C. A. Fenstermacher ◽  
R. G. Bennett ◽  
A. E. Walters ◽  
C. K. Bockelman ◽  
H. L. Schultz
1958 ◽  
Vol 111 (3) ◽  
pp. 906-912 ◽  
Author(s):  
J. E. Draper ◽  
C. A. Fenstermacher ◽  
H. L. Schultz

1972 ◽  
Vol 185 (1) ◽  
pp. 229-235 ◽  
Author(s):  
H. Weigmann ◽  
G. Rohr ◽  
M. Heske

1976 ◽  
Vol 54 (4) ◽  
pp. 383-389 ◽  
Author(s):  
V. J. Thomson ◽  
W. V. Prestwich ◽  
T. J. Kennett

Measurement of gamma rays following neutron capture has revealed resonances at 29, 67, 85, and 173 keV for the 28Si(n,γ)29Si reaction, and 16 and 35 keV for the 29Si(n,γ)30Si reaction. The characteristics of the resonance decay properties are discussed. Both the 67 and 85 keV resonances appear to result from p wave capture.


1976 ◽  
Vol 14 (1) ◽  
pp. 75-91 ◽  
Author(s):  
David L. Bushnell ◽  
Gianni R. Tassotto ◽  
Robert K. Smither

1970 ◽  
Vol 2 (3) ◽  
pp. 1115-1125 ◽  
Author(s):  
M. R. Bhat ◽  
R. E. Chrien ◽  
D. I. Garber ◽  
O. A. Wasson

1975 ◽  
Vol 68 ◽  
pp. 363-383 ◽  
Author(s):  
R. Ramaty ◽  
R. E. Lingenfelter

We have treated in detail the theory of gamma-ray line production in solar flares. The strongest line, both predicted theoretically and detected observationally at 2.2 MeV, is due to neutron capture by protons in the photosphere. The neutrons are produced in nuclear reactions of flare accelerated particles which also produce positrons and prompt nuclear gamma rays. From the comparison of the observed and calculated intensities of the lines at 4.4 or 6.1 MeV to that of the 2.2 MeV line it is possible to deduce the spectrum of accelerated nuclei in the flare region; and from the absolute intensities of these lines it is possible to obtain the total number of accelerated nuclei at the Sun. The study of the 2.2 MeV line also gives information on the amount of He3 in the photosphere. The study of the line at 0.51 MeV resulting from positron annihilation complements the data obtained from the other lines; in addition it gives information on the temperature and density in the annihilation region and on the anisotropy of the accelerated electron beam which produces continuum gamma rays at energies greater than about 1 MeV.


1967 ◽  
Vol 158 (4) ◽  
pp. 1049-1062 ◽  
Author(s):  
I. Bergqvist ◽  
J. A. Biggerstaff ◽  
J. H. Gibbons ◽  
W. M. Good

1977 ◽  
Vol 281 (2) ◽  
pp. 240-260 ◽  
Author(s):  
M. Stefanon ◽  
F. Corvi

1974 ◽  
Vol 233 (1) ◽  
pp. 185-216 ◽  
Author(s):  
F. Corvi ◽  
M. Stefanon

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