2011
DOI: 10.1103/physreva.83.042707
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Photoassociation of a cold-atom-molecule pair. II. Second-order perturbation approach

Abstract: The electrostatic interaction between an excited atom and a diatomic ground state molecule in an arbitrary rovibrational level at large mutual separations is investigated with a general second-order perturbation theory, in the perspective of modeling the photoassociation between cold atoms and molecules. We find that the combination of quadrupole-quadrupole and van der Waals interactions compete with the rotational energy of the dimer, limiting the range of validity of the perturbative approach to distances la… Show more

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Cited by 18 publications
(28 citation statements)
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References 31 publications
(29 reference statements)
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“…2(b), where the influence of the spin-orbit interaction of O( 3 P 2 ) on the anisotropy of the PES is clearly visible. The calculations presented in this section are based on our previous work on Cs(6p 2 P )- [25,[43][44][45] The quantities regarding the oxygen atom are expressed here in the fine-structure basis |J a M a and are identical to those of Section II. To stress the differences with the fixedgeometry problem for the diatom, all the quantities X that are averaged over O 2 vibrational wave functions are overlined (X).…”
Section: B Asymptotic Pess: Results and Discussionmentioning
confidence: 99%
“…2(b), where the influence of the spin-orbit interaction of O( 3 P 2 ) on the anisotropy of the PES is clearly visible. The calculations presented in this section are based on our previous work on Cs(6p 2 P )- [25,[43][44][45] The quantities regarding the oxygen atom are expressed here in the fine-structure basis |J a M a and are identical to those of Section II. To stress the differences with the fixedgeometry problem for the diatom, all the quantities X that are averaged over O 2 vibrational wave functions are overlined (X).…”
Section: B Asymptotic Pess: Results and Discussionmentioning
confidence: 99%
“…Our work extends the results in Refs. [20][21][22] to fine structure states with high n, as relevant for Rydberg states.…”
Section: Methodsmentioning
confidence: 99%
“…, one retrieves the product of the multipole polarizabilities at imaginary frequencies. The term −2a/(b 2 − a 2 ) = 2a/(a 2 − b 2 ) results in the dynamic polarizability of partner A, taken at the real frequencies corresponding to the transitions from |β B J B to lower-energy levels of partner B [42,43]. Finally the dispersion effective operator readŝ…”
Section: Dispersion Energymentioning
confidence: 99%