1966
DOI: 10.1063/1.3048129
|View full text |Cite
|
Sign up to set email alerts
|

The Theory of Electron–Atom Collisions

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
11
0
1

Year Published

1968
1968
2022
2022

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 12 publications
(12 citation statements)
references
References 0 publications
0
11
0
1
Order By: Relevance
“…(11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24)(25)(26)(27)(28)(29) into the above expressions gives after using eqs. (11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24)(25) and (II-50),…”
Section: Appendix a Derivation Of Equation (Ll-i42)unclassified
See 4 more Smart Citations
“…(11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24)(25)(26)(27)(28)(29) into the above expressions gives after using eqs. (11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24)(25) and (II-50),…”
Section: Appendix a Derivation Of Equation (Ll-i42)unclassified
“…By using the gauge in which the scalar potential vanishes, the electric field E(r;, t) can be described by a vector potential A(r, t) through the relationship With J(r) defined as eq. (11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24)(25)(26)(27)(28). When the medium is acted upon by the field A(r,t), the total current operator at thp time t becomes J(r,t) = J(r)+J A (r,t).…”
Section: Dt (Ii-u6)mentioning
confidence: 99%
See 3 more Smart Citations