Cross section and analyzing power measurements for the giant resonance region inPb208with 200-MeV protons

1986 ◽  
Vol 33 (6) ◽  
pp. 1943-1954 ◽  
Author(s):  
D. K. McDaniels ◽  
J. R. Tinsley ◽  
J. Lisantti ◽  
D. M. Drake ◽  
I. Bergqvist ◽  
...  
1986 ◽  
Vol 33 (1) ◽  
pp. 22-30 ◽  
Author(s):  
D. W. Miller ◽  
J. D. Brown ◽  
D. L. Friesel ◽  
W. W. Jacobs ◽  
W. P. Jones ◽  
...  

1982 ◽  
Vol 25 (3) ◽  
pp. 1263-1271 ◽  
Author(s):  
S. Kailas ◽  
P. P. Singh ◽  
A. D. Bacher ◽  
C. C. Foster ◽  
D. L. Friesel ◽  
...  

1983 ◽  
Vol 406 (2) ◽  
pp. 257-268 ◽  
Author(s):  
T.J. Boal ◽  
E.G. Muirhead ◽  
D.J.S. Findlay

2007 ◽  
Vol 76 (1) ◽  
Author(s):  
Y. Maeda ◽  
H. Sakai ◽  
K. Fujita ◽  
M. B. Greenfield ◽  
K. Hatanaka ◽  
...  

1960 ◽  
Vol 38 (2) ◽  
pp. 231-239 ◽  
Author(s):  
J. D. King ◽  
R. N. H. Haslam ◽  
R. W. Parsons

The reaction N14(γ,n)N13 has been studied by irradiating dicyandiamide in the X-ray beam of a 25-Mev betatron and measuring the residual activity with a sodium iodide crystal system. The photoneutron cross section shows maxima at 11.7, 13.2, 15.2, 19.5, and 22.8 Mev, the last two being in the giant resonance region. The integrated cross section from threshold to the beginning of the giant resonance region is 1.8 Mev-mb, and this is compared with a recent theoretical prediction. During the course of the experiment, accurate measurements were made of the half-life of N13 and it was found to be 9.93 ± 0.05 minutes.


1989 ◽  
Vol 39 (1) ◽  
pp. 65-69 ◽  
Author(s):  
R. Abegg ◽  
D. A. Hutcheon ◽  
C. A. Miller ◽  
L. Antonuk ◽  
J. M. Cameron ◽  
...  

2000 ◽  
Vol 663-664 ◽  
pp. 545c-548c ◽  
Author(s):  
B.D. Anderson ◽  
O. Osadchy ◽  
J. Sowinski ◽  
A.R. Baldwin ◽  
W. Franklin ◽  
...  

1965 ◽  
Vol 17 (1) ◽  
pp. 49-50 ◽  
Author(s):  
B.S. Dolbilkin ◽  
V.I. Korin ◽  
L.E. Lazareva ◽  
F.A. Nikolaev

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