Corrigendum to ‘Dissociative electron impact ionization of methyl tert-butyl ether: Total ionization cross-section and kinetic energy distributions’ [Chem. Phys. Lett. 400 (2004) 191–195]

2005 ◽  
Vol 413 (4-6) ◽  
pp. 512
Author(s):  
T.M. Di Palma ◽  
B. Apicella ◽  
M. Armenante ◽  
R. Velotta ◽  
X. Wang ◽  
...  
1969 ◽  
Vol 184 (1) ◽  
pp. 242-244 ◽  
Author(s):  
K. C. Mathur ◽  
A. N. Tripathi ◽  
S. K. Joshi

2007 ◽  
Vol 76 (3) ◽  
pp. 521-523
Author(s):  
F.F. Chipev ◽  
A.A. Borovik ◽  
I.V. Chernyshova ◽  
J.E. Kontros ◽  
O.B. Shpenik

2019 ◽  
Vol 150 (6) ◽  
pp. 064313 ◽  
Author(s):  
Dhanoj Gupta ◽  
Heechol Choi ◽  
Suvam Singh ◽  
Paresh Modak ◽  
Bobby Antony ◽  
...  

1961 ◽  
Vol 16 (6) ◽  
pp. 583-598 ◽  
Author(s):  
F. B. Malik ◽  
E. Trefftz

The ionization cross-section of highly ionized oxygen, O4+, is calculated according to the “distorted-wave” method. Exchange between the scattered and the ejected electron is taken into account as far as it is of long range nature. It is shown that contributions of high total angular momentum L are essential, L=0 giving only 3% of the total cross-section. This result should qualitatively be the same for all highly ionized atoms, whereas the following seems to be a special feature of O V ionization: for energies around twice the ionization energy the contributions of the optically allowed transitions of the ejected electron (angular momentum lej=1) are relatively small. The contributions of lej =0, 1, 2 and 3 are about 16%, 18%, 24% and 19% respectively for E=20.13.6 eV=2.39 × Ionization energy. The maximum cross section is 0.112 at. u. = 0.31 ·10-18 cm2 for electrons of 310 eV kinetic energy (2.8 × ionization energy). It is about twice as large as given by the ELWERT formula.


Sign in / Sign up

Export Citation Format

Share Document