2014
DOI: 10.1063/1.4904265
|View full text |Cite
|
Sign up to set email alerts
|

New observation and combined analysis of the Cs2g−, u+, and 1g states at the asymptotes 6S1/2 + 6P1/2 and 6S1/2 + 6P3/2

Abstract: We report on new observations of the photoassociation spectroscopy of ultracold cesium molecules using a highly sensitive detection technique and a combined analysis with all observed electronic states. The technique is achieved by directly modulating the frequency of the trapping lasers of a magneto-optical trap. New observations of the Cs2 0g(-), 0u(+), and 1g states at the asymptotes 6S1/2 + 6P1/2 and 6S1/2 + 6P3/2 are reported. The spectral range is extended to the red detuning of 112 cm(-1) below the 6S1/… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
9
0

Year Published

2016
2016
2019
2019

Publication Types

Select...
3
3
1

Relationship

2
5

Authors

Journals

citations
Cited by 22 publications
(9 citation statements)
references
References 36 publications
0
9
0
Order By: Relevance
“…The PA spectroscopy is measured by detecting the loss of Cs atoms optically trapped in a crossed ODT as a function of PA laser frequency. If the PA laser frequency is resonant with the energy difference between the scattering state of colliding atomic pairs and the bound excited state of diatomic molecule in a particular rovibrational level, the pure long-range state Cs 2 molecule is produced in the outer well of the double–well potential of the ( ) state 26 , 27 . Figure 1 shows a typical PA spectrum of the rovibrational level , of the electronically excited state of Cs 2 .…”
Section: Resultsmentioning
confidence: 99%
“…The PA spectroscopy is measured by detecting the loss of Cs atoms optically trapped in a crossed ODT as a function of PA laser frequency. If the PA laser frequency is resonant with the energy difference between the scattering state of colliding atomic pairs and the bound excited state of diatomic molecule in a particular rovibrational level, the pure long-range state Cs 2 molecule is produced in the outer well of the double–well potential of the ( ) state 26 , 27 . Figure 1 shows a typical PA spectrum of the rovibrational level , of the electronically excited state of Cs 2 .…”
Section: Resultsmentioning
confidence: 99%
“…[24,25], has a potential curve with a distinct double-well shape, with a deep inner well with an equilibrium distance of roughly 10 a.u. and a shallow outer well caused by the competition between the long-range electrostatic interaction between the 6s and the 6p atoms (varying as R −3 , where R is the internuclear distance) and the spin-orbit interaction, which couples the (1) 3 Σ + g (6s+6p) state and the (1) 3 Π g (6s + 6p) state.…”
Section: Molecules In the Triplet Statementioning
confidence: 99%
“…However, deeply bound ground state molecules may be produced through decay in some exceptional systems [53,54,160] [52,[161][162][163][164][165][166].…”
Section: Photoassociationmentioning
confidence: 99%