Cross sections for the ionisation of helium by electron impact in a distorted-wave model

1979 ◽  
Vol 12 (7) ◽  
pp. 1267-1278 ◽  
Author(s):  
B H Bransden ◽  
J J Smith ◽  
K H Winters
1977 ◽  
Vol 55 (12) ◽  
pp. 1074-1082 ◽  
Author(s):  
K. H. Winters ◽  
M. Issa ◽  
B. H. Bransden

Angular distributions and (x, λ) angular correlation parameters are calculated in the generalized distorted wave model of Bransden and Issa for 31P excitation of helium in the energy interval 100 to 500 eV. Comparison is made with the experimental data at 100 eV and with the results of the theoretical models. Angular distributions are also presented for the excitation of the 31S and 31D levels, for which a comparison with data is not yet possible.


1989 ◽  
Vol 39 (9) ◽  
pp. 4509-4517 ◽  
Author(s):  
Wen-Jia Qian ◽  
Yong-Ki Kim ◽  
Jean-Paul Desclaux

2007 ◽  
Vol 24 (3) ◽  
pp. 691-694 ◽  
Author(s):  
Jiang Jun ◽  
Dong Chen-Zhong ◽  
Xie Lu-You ◽  
Wang Jian-Guo ◽  
Yan Jun ◽  
...  

2011 ◽  
Vol 89 (6) ◽  
pp. 723-727 ◽  
Author(s):  
Mohammed Sahlaoui ◽  
Mammar Bouamoud

Theoretical triple differential cross sections for the electron-impact ionization of water molecules at high incident energy are presented. The results are derived using an analytical expression for the transition amplitude in the framework of the one Coulomb wave model. For accurate comparison with experiments, an average of the cross sections on the random orientations of the target has been used. The comparison of our results with the available experimental measurements shows that our formalism is able to describe the water molecule ionization process with good precision. The present approach can be used to describe the ionization of other molecular targets with chemical form XHn by other charged particles.


Cross-sections for excitation of the 2 3 P state of helium from the ground state have been calculated by the distorted-wave method. The polarization of radiation emitted as a result of the excitation is also calculated. Comparison is made with the corresponding results given by the Born—Oppenheimer approximation. Although there are considerable differences at electron energies below 100 eV these are much less marked than for the excitation of the 2 3 S state. The distorted wave method gives cross-sections in closer agreement with observation but substantial discrepancies still remain. It is difficult, however, to estimate their magnitude with any certainty because there are inconsistencies in the observed data.


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