INELASTIC AND ANOMALOUS ELASTIC SCATTERING OF 88.03 keV GAMMA RAYS

1987 ◽  
Vol 48 (C9) ◽  
pp. C9-835-C9-837
Author(s):  
P. P. KANE ◽  
G. BASAVARAJU ◽  
S. M. LAD ◽  
K. M. VARIER ◽  
L. KISSELL ◽  
...  
1978 ◽  
Vol 11 (23) ◽  
pp. 3969-3975 ◽  
Author(s):  
M Satyendra Prasad ◽  
G Kusa Raju ◽  
K Narasimha Murty ◽  
V A Narasimha Murty ◽  
V Lakshminarayana

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.


1966 ◽  
Vol 195 (3) ◽  
pp. 252-272 ◽  
Author(s):  
Ulrich Hauser ◽  
Bernd Mussgnug

1971 ◽  
Vol 34 (6) ◽  
pp. 494-496 ◽  
Author(s):  
R. Moreh ◽  
D. Salzmann ◽  
G. Ben-David

1956 ◽  
Vol 101 (1) ◽  
pp. 4-8 ◽  
Author(s):  
A. K. Mann

1968 ◽  
Vol 46 (10) ◽  
pp. 1153-1161 ◽  
Author(s):  
W. R. Dixon ◽  
R. S. Storey

The elastic scattering of 60Co gamma rays from lead has been remeasured using a lithium-drifted germanium detector. For angles less than 90°, there is satisfactory agreement between the measured and calculated values. For angles greater than 90°, the measured values are significantly smaller. The discrepancy is too large to be attributed to destructive interference from Delbrück scattering. An explanation can be found in the possibility that there are phase shifts between the Rayleigh and nuclear Thomson components.


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