1982
DOI: 10.1016/0167-5087(82)90388-x
|View full text |Cite
|
Sign up to set email alerts
|

Collinear fast-beam laser spectroscopy experiment: Measurement of hyperfine structure and isotope shifts in Xe II

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
7
0

Year Published

1985
1985
2014
2014

Publication Types

Select...
4
2
2

Relationship

0
8

Authors

Journals

citations
Cited by 17 publications
(7 citation statements)
references
References 8 publications
0
7
0
Order By: Relevance
“…1b (again, the other six are of the same transition shown for the even isotopes). The hyperfine splitting constants are only known for a limited set of energy levels [16][17][18][19][20]. While isotope shifts and all of the hyperfine splitting constants are available for the upper and lower levels of the neutral 823.2 nm transition, the 834.7 nm xenon ion transition only has data on the nuclear spin splitting constants of the upper state, and no information is available on the transitiondependent isotope shifts.…”
Section: Xenon Spectroscopymentioning
confidence: 99%
“…1b (again, the other six are of the same transition shown for the even isotopes). The hyperfine splitting constants are only known for a limited set of energy levels [16][17][18][19][20]. While isotope shifts and all of the hyperfine splitting constants are available for the upper and lower levels of the neutral 823.2 nm transition, the 834.7 nm xenon ion transition only has data on the nuclear spin splitting constants of the upper state, and no information is available on the transitiondependent isotope shifts.…”
Section: Xenon Spectroscopymentioning
confidence: 99%
“…Unfortunately experimental data for the isotope shift of the 5d 2 F 7/2  6p 2 D 0 5/2 transition is not available. Following the approach of Manzella 6) and others experimental data of the similar 5d 4 D 7/2  6p 4 P 0 5/2 was used 7,8) . Further splitting into a hyperfine structure occurs for the isotopes with non-zero nuclear spin, Xe 129 and Xe 131 , due to nucleon-electron spin interaction producing a total of 19 lines.…”
Section: Hyperfine Structurementioning
confidence: 99%
“…Each of these isotopes causes a slightly different transition energy E ij , resulting in isotopic splitting. Both of the computational models in this study use naturally-occurring xenon isotopic abundances, 15 while we take isotopic shifts (conventionally defined relative to the center frequency for 132 Xe) for the 5d 4 D 7/2 − 6p 4 P 0 5/2 transition at 605.1 nm from the fast ion-beam LIF surveys of Bingham et al 16 and Borghs et al 17 Seven of the nine stable isotopes of xenon have even atomic mass, resulting in no nuclear spin I. The two isotopes with an odd atomic mass, however, have non-zero nuclear spin quantum numbers I.…”
Section: /2mentioning
confidence: 99%
“…transition taken from the fast ion-beam LIF surveys of Bingham et al 16 and Borghs et al 17 Figure 2(a) shows the 605.1 nm absorption spectrum for a perfectly cold stationary plasma, where the velocity distribution f (v) = δ(v). This can be described by the convolution…”
Section: /2mentioning
confidence: 99%