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Physical Review A

Weakly bound 87 Rb 2 (5s1/2+5p1/2)1g molecules: Hyperfine interaction and LeRoy-Bernstein analysis including linear and nonlinear terms

Haikel Jelassi, Laurence Pruvost

Published Mar 20, 2014• 10 citations
Publisher

Abstract

Data on the $(5{s}_{1/2}+5{p}_{1/2}){1}_{g}$ ${}^{87}{\text{Rb}}_{2}$ state under the ${D}_{1}$ limit, provided by a photoassociation experiment on cold atoms, have been analyzed by an improved LeRoy-Bernstein (LRB) approach including linear and nonlinear terms and provide a ${c}_{6}$ value of the potential. To do that, using a model for hyperfine structure shifts, we have first subtracted the hyperfine effects in the split lines and deduced the vibrational energies. Then, we have compared three LRB-type models to fit the data. We conclude that the second-order improved LRB is well suited and allows us to deduce an experimental value of ${c}_{6}$ [${c}_{6}=(15.14\ifmmode\pm\else\textpm\fi{}0.05)\ifmmode\times\else\texttimes\fi{}{10}^{4}$ a.u.].

DOI
10.1103/physreva.89.032514

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Data on the (5s1/2+5p1/2)1g(5{s}_{1/2}+5{p}_{1/2}){1}_{g}(5s1/2​+5p1/2​)1g​ 87Rb2{}^{87}{\text{Rb}}_{2}87Rb2​ state under the D1{D}_{1}D1​ limit, provided by a photoassociation experiment on cold atoms, have been analyzed by an improved LeRoy-Bernstein (LRB) approach including linear and nonlinear terms and provide a c6{c}_{6}c6​ value of the potential. To do that, using a model for hyperfine structure shifts, we have first subtracted the hyperfine effects in the split lines and deduced the vibrational energies. Then, we have compared three LRB-type models to fit the data. We conclude that the second-order improved LRB is well suited and allows us to deduce an experimental value of c6{c}_{6}c6​ [c6=(15.14\ifmmode±\else\textpm\fi0.05)\ifmmode×\else\texttimes\fi104{c}_{6}=(15.14\ifmmode\pm\else\textpm\fi{}0.05)\ifmmode\times\else\texttimes\fi{}{10}^{4}c6​=(15.14\ifmmode±\else\textpm\fi0.05)\ifmmode×\else\texttimes\fi104 a.u.].
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