scholarly journals Electron-impact ionization of atomic hydrogen

2001 ◽  
Vol 63 (2) ◽  
Author(s):  
M. Baertschy ◽  
T. N. Rescigno ◽  
W. A. Isaacs ◽  
X. Li ◽  
C. W. McCurdy
1988 ◽  
Vol 66 (5) ◽  
pp. 399-401 ◽  
Author(s):  
K. K. Mukherjee ◽  
P. S. Mazumdar ◽  
S. Brajamani

The total cross-section for electron-impact ionization from the ground state of atomic hydrogen is studied by using the distorted-wave polarized orbital method. In the present calculation we have taken into account the matrix elements arising from the distorted part of the target wave function. The present results are in good agreement with experimental findings.


1963 ◽  
Vol 81 (2) ◽  
pp. 375-378 ◽  
Author(s):  
S Geltman ◽  
M R H Rudge ◽  
M J Seaton

2003 ◽  
Vol 68 (3) ◽  
Author(s):  
J. G. Childers ◽  
K. E. James ◽  
M. Hughes ◽  
Igor Bray ◽  
M. Baertschy ◽  
...  

Atoms ◽  
2020 ◽  
Vol 8 (2) ◽  
pp. 26
Author(s):  
C. DeMars ◽  
S. Ward ◽  
J. Colgan ◽  
S. Amami ◽  
D. Madison

We investigate ionization of atomic hydrogen by electron- and positron-impact. We apply the Coulomb–Born (CB1) approximation, various modified CB1 approximations, the three body distorted wave (3DW) approximation, and the time-dependent close-coupling (TDCC) method to electron-impact ionization of hydrogen. For electron-impact ionization of hydrogen for an incident energy of approximately 76.45 eV, we obtain a deep minimum in the CB1 triply differential cross section (TDCS). However, the TDCC for 74.45 eV and the 3DW for 74.46 eV gave a dip in the TDCS. For positron-hydrogen ionization (breakup) we apply the CB1 approximation and a modified CB1 approximation. We obtain a deep minimum in the TDCS and a zero in the CB1 transition matrix element for an incident energy of 100 eV with a gun angle of 56.13 ° . Corresponding to a zero in the CB1 transition matrix element, there is a vortex in the velocity field associated with this element. For both electron- and positron-impact ionization of hydrogen the velocity field rotates in the same direction, which is anticlockwise. All calculations are performed for a doubly symmetric geometry; the electron-impact ionization is in-plane and the positron-impact ionization is out-of-plane.


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