2009
DOI: 10.1016/j.jms.2009.06.004
|View full text |Cite
|
Sign up to set email alerts
|

Time-resolved study of the A2Π state of CaH by laser spectroscopy

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

0
6
0

Year Published

2012
2012
2023
2023

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 13 publications
(7 citation statements)
references
References 24 publications
(38 reference statements)
0
6
0
Order By: Relevance
“…FCFs and VBRs for the measured transitions of CaH. The experimental radiative lifetime for the A state was obtained from reference [49] and for the B state from reference [50]. The excited state vibrational quantum number is always ν = 0.…”
Section: Vibrational Branching Ratio Measurementmentioning
confidence: 99%
“…FCFs and VBRs for the measured transitions of CaH. The experimental radiative lifetime for the A state was obtained from reference [49] and for the B state from reference [50]. The excited state vibrational quantum number is always ν = 0.…”
Section: Vibrational Branching Ratio Measurementmentioning
confidence: 99%
“…To our knowledge there are no experimental absolute intensity measurements of CaH. However, a few lifetime measurements for a number of low‐lying vibrational states v = 0, 1, 2 of the X , A and B states were used to estimate the corresponding oscillator strengths or Einstein coefficients (Klynning et al ; Berg, Ekvall & Kelly ; Liu et al ). The permanent electric dipole moments of CaH were obtained experimentally for a few low electronic states using the Stark effect (Steimle, Chen & Gengler ; Chen & Steimle ).…”
Section: Introductionmentioning
confidence: 99%
“…Previous studies revealed the laser cooling features of AEMHs in the following aspects: (i) highly diagonal Franck–Condon factor (FCF) that describes the overlap of vibrational wave functions involved in the cooling optical transition ( A 2 Π 1/2 ← X 2 Σ + ); (ii) short radiative lifetime of the A 2 Π 1/2 state ( 9 BeH: 81 ns, 24 MgH: 43.6 ns, 40 CaH: 33.2 ns, 88 SrH: 33.8 ns, and 138 BaH: 136.5 ns , ), which corresponds to strong spontaneous radiation decay rate; (iii) no intervening electronic states (except BaH) in the X 2 Σ + ← A 2 Π 1/2 transition. Recently, BaH has been extensively examined by Zelevinsky et al both theoretically via ab initio calculations and experimentally via spectroscopic detection and direct laser cooling. They obtained vibrational branching ratios for B 2 Σ + – X 2 Σ + and A 2 Π 1/2 – X 2 Σ + optical cycling transitions using fluorescence and absorption detection, confirming the A 2 Π 1/2 state as a superior choice for laser cooling rather than the B 2 Σ + state, based on which Zelevinsky et al adopted A 2 Π 1/2 ← X 2 Σ + as the optical cycling transition while repumping excited vibrational levels of the ground state through the B 2 Σ + state.…”
Section: Introductionmentioning
confidence: 99%