Internal-conversion coefficient determination of odd parity for the 108.8-keV first-excited state ofRb91

1975 ◽  
Vol 11 (4) ◽  
pp. 1455-1458 ◽  
Author(s):  
F. K. Wohn ◽  
W. L. Talbert ◽  
R. S. Weinbeck ◽  
M. D. Glascock ◽  
J. K. Halbig
1997 ◽  
Vol 55 (4) ◽  
pp. 1665-1675 ◽  
Author(s):  
F. Attallah ◽  
M. Aiche ◽  
J. F. Chemin ◽  
J. N. Scheurer ◽  
W. E. Meyerhof ◽  
...  

2014 ◽  
Vol 87 ◽  
pp. 192-194 ◽  
Author(s):  
Izabela T. Matos ◽  
Marina F. Koskinas ◽  
Tatiane S. Nascimento ◽  
Ione M. Yamazaki ◽  
Mauro S. Dias

1. Introduction .—The Internal Conversion Coefficient of γ-rays has recently been calculated by Hulme and by Taylor and Mott. The assumptions on which both of these calculations rest may be analysed as follows. I.—A nucleus, originally in an excited state of energy W n , radiates, corresponding to the transition to each lower state of energy W m , an electromagnetic field which may be either that of a dipole or that of a quadripole. For a dipole such a field has scalar and vector potentials given by


1986 ◽  
Vol 91 (4) ◽  
pp. 352-358 ◽  
Author(s):  
N. Venkateswara Rao ◽  
Ch. Suryanarayana ◽  
D. G. S. Narayana ◽  
S. Bhuloka Reddy ◽  
G. Satynarayana ◽  
...  

1949 ◽  
Vol 27a (2) ◽  
pp. 17-25 ◽  
Author(s):  
J. P. Stanley

Hulme's formula for the internal conversion of γ-radiation is simplified and used to calculate the internal conversion coefficient in the electric dipole case for electrons in the K-shell. For each of the elements Z = 69, 74, 79, 84, 89, IK is calculated for 10 values of the variable [Formula: see text] and a table obtained by interpolation is given for θ = 0.05 to θ = 1.70.


1960 ◽  
Vol 16 (1) ◽  
pp. 175-187 ◽  
Author(s):  
J. Lindskog ◽  
E. Bashandy ◽  
T.R. Gerholm

1977 ◽  
Vol 3 (12) ◽  
pp. L267-L270 ◽  
Author(s):  
C J Lister ◽  
A M Al-Naser ◽  
M J Maynard ◽  
P J Nolan

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