Abstract
Atom excitation in collisions with fully stripped ions at intermediate and high energies is studied in the framework of the semiclassical sudden-Born approximation. Two different scaling rules are manifested for transitions in the target-atom with even and odd numbers of {Delta}{sub fi}=l{sub f}+m{sub f}-l{sub i}-m{sub i} where l{sub i}, m{sub i} and l{sub f}, m{sub f} are the orbital and magnetic quantum numbers of the initial and the final states respectively. 18 refs.; 3 figs.; 3 tabs.
Citation Formats
Klintsov, V N, and Yudin, G L.
Scaling in the processes of ion-atom excitation; Skejling v protsessakh ion-atomnogo vozbuzhdeniya.
USSR: N. p.,
1991.
Web.
Klintsov, V N, & Yudin, G L.
Scaling in the processes of ion-atom excitation; Skejling v protsessakh ion-atomnogo vozbuzhdeniya.
USSR.
Klintsov, V N, and Yudin, G L.
1991.
"Scaling in the processes of ion-atom excitation; Skejling v protsessakh ion-atomnogo vozbuzhdeniya."
USSR.
@misc{etde_10136069,
title = {Scaling in the processes of ion-atom excitation; Skejling v protsessakh ion-atomnogo vozbuzhdeniya}
author = {Klintsov, V N, and Yudin, G L}
abstractNote = {Atom excitation in collisions with fully stripped ions at intermediate and high energies is studied in the framework of the semiclassical sudden-Born approximation. Two different scaling rules are manifested for transitions in the target-atom with even and odd numbers of {Delta}{sub fi}=l{sub f}+m{sub f}-l{sub i}-m{sub i} where l{sub i}, m{sub i} and l{sub f}, m{sub f} are the orbital and magnetic quantum numbers of the initial and the final states respectively. 18 refs.; 3 figs.; 3 tabs.}
place = {USSR}
year = {1991}
month = {Dec}
}
title = {Scaling in the processes of ion-atom excitation; Skejling v protsessakh ion-atomnogo vozbuzhdeniya}
author = {Klintsov, V N, and Yudin, G L}
abstractNote = {Atom excitation in collisions with fully stripped ions at intermediate and high energies is studied in the framework of the semiclassical sudden-Born approximation. Two different scaling rules are manifested for transitions in the target-atom with even and odd numbers of {Delta}{sub fi}=l{sub f}+m{sub f}-l{sub i}-m{sub i} where l{sub i}, m{sub i} and l{sub f}, m{sub f} are the orbital and magnetic quantum numbers of the initial and the final states respectively. 18 refs.; 3 figs.; 3 tabs.}
place = {USSR}
year = {1991}
month = {Dec}
}