2008
DOI: 10.1016/j.physleta.2008.04.059
|View full text |Cite
|
Sign up to set email alerts
|

Two photon resonant excitation of Copper–Rydberg levels

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

1
0
0

Year Published

2013
2013
2014
2014

Publication Types

Select...
2

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(1 citation statement)
references
References 26 publications
1
0
0
Order By: Relevance
“…In the present work, we saw up to n = 16 clearly, with a weak feature for n = 17 sometimes visible, while Castleberry et al 8 saw from n = 9 up to n = 21, with an intensity distribution similar to that in Fig. 1 16 The important selection rules for the two-photon processes include orbital angular momentum change ∆l=0, ±2, where l is the orbital angular momentum quantum number of the electron being excited (s  s is also explicitly forbidden); whereas the total angular momentum change must be ∆J = 0, ±1, ±2, with the total electronic spin remaining unchanged if LS-coupling prevails.…”
Section: Resultssupporting
confidence: 58%
“…In the present work, we saw up to n = 16 clearly, with a weak feature for n = 17 sometimes visible, while Castleberry et al 8 saw from n = 9 up to n = 21, with an intensity distribution similar to that in Fig. 1 16 The important selection rules for the two-photon processes include orbital angular momentum change ∆l=0, ±2, where l is the orbital angular momentum quantum number of the electron being excited (s  s is also explicitly forbidden); whereas the total angular momentum change must be ∆J = 0, ±1, ±2, with the total electronic spin remaining unchanged if LS-coupling prevails.…”
Section: Resultssupporting
confidence: 58%