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Journal of Physics B Atomic Molecular and Optical Physics

Photoassociation of85Rb atoms into 0u+states near the 5S+5P atomic limits

T. H. Bergeman, J Qi, Dajun Wang, Yanyan Huang, Hyewon Pechkis, Edward E. Eyler, P. L. Gould, William C. Stwalley, Robert A. Cline, Joseph D. Miller, Daniel J. Heinzen

Published Sep 25, 2006• 53 citations
Publisher

Abstract

New photoassociation data on the 0u+ levels of Rb2 below the 5S+5P1/2 limit are combined with older data (Cline et al 1994 Phys. Rev. Lett. 73 632) in a fit to potentials and spin–orbit functions. The P1/2 data exhibit oscillations in the B(v) values due to coupling between the two 0u+ series, as modelled accurately by a coupled potentials approach. The fitted value for the C3 dispersion parameter from the combined data agrees well with the value derived from the pure long-range 0g− state.

DOI
10.1088/0953-4075/39/19/s01

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Long range Rb{sub 2} excited state dispersion interactions and transition dipole moment from photoassociation spectra

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Hyperfine and vibrational structure of weakly bound levels of the lowest 1g state of molecular 87 Rb 2

Chin‐Chun Tsai, T. H. Bergeman, Eite Tiesinga +2 more

Photoassociation resonances in the ${}^{87}$Rb${}_{2}$ ${1}_{g}$ state dissociating to $5{\phantom{\rule{0.16em}{0ex}}}^{2}S+5{}^{2}{P}_{1/2}$ were produced by the excitation of colliding ${}^{87}$Rb atoms in a far-off resonance trap. Levels down to 31 cm${}^{\ensuremath{-}1}$ below the dissociation limit were measured with resonance linewidths of 15 to 20 MHz, and have been located to a one-sigma combined systematic and statistical uncertainty of 50 MHz relative to the $5{\phantom{\rule{0.16em}{0ex}}}^{2}S+5{}^{2}{P}_{1/2}$ limit. Electron and nuclear spins were fixed to a space-fixed axis by circularly polarized optical pumping, so that only states with total nuclear spin $I=3$ were excited, thereby greatly simplifying the spectrum. The analysis of the data yielded hyperfine coupling parameters $A(v)$, vibrational $G(v)$, and rotational $B(v)$ parameters. The $G(v)$ parameters could be fit to an rms accuracy of about 0.01 cm${}^{\ensuremath{-}1}$ to a potential constructed from current ${C}_{3}$ and ${C}_{6}$ long-range dispersion parameters plus an ab initio potential that was adjusted in depth and with quadratic terms in the internuclear distance added to the inner wall.

Physical Review A•Nov 13, 2013•4 citations
New photoassociation data on the 0u+ levels of Rb2 below the 5S+5P1/2 limit are combined with older data (Cline et al 1994 Phys. Rev. Lett. 73 632) in a fit to potentials and spin–orbit functions. The P1/2 data exhibit oscillations in the B(v) values due to coupling between the two 0u+ series, as modelled accurately by a coupled potentials approach. The fitted value for the C3 dispersion parameter from the combined data agrees well with the value derived from the pure long-range 0g− state.
We report on photoassociation of cold 87Rb^{87}\mathrm{Rb}87Rb atoms providing the spectroscopy of (5s1∕2+5p1∕2)0u+(5{s}_{1∕2}+5{p}_{1∕2}){0}_{u}^{+}(5s1∕2​+5p1∕2​)0u+​ long-range molecular states, in the energy range of [$\ensuremath{-}12.5$, $\ensuremath{-}0.7\phantom{\rule{0.3em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}1}$] below the dissociation limit. A Lu-Fano approach coupled to the LeRoy-Bernstein formula is used to analyze the data. The Lu-Fano graph exhibits the coupling of the molecular series with the (5s1∕2+5p3∕2)0u+(5{s}_{1∕2}+5{p}_{3∕2}){0}_{u}^{+}(5s1∕2​+5p3∕2​)0u+​ one, which is due to spin effects in the molecule. A two-channel model involving an improved LeRoy-Bernstein formula allows us to characterize the molecular series, to localize (5s1∕2+5p3∕2)0u+(5{s}_{1∕2}+5{p}_{3∕2}){0}_{u}^{+}(5s1∕2​+5p3∕2​)0u+​ levels, to evaluate the coupling, and to predict the energy and width of the first predissociated level of (5s1∕2+5p3∕2)0u+(5{s}_{1∕2}+5{p}_{3∕2}){0}_{u}^{+}(5s1∕2​+5p3∕2​)0u+​ series. An experimental spectrum confirms the prediction.
Numerical calculations of vibrational levels of alkali dimers close to the dissociation limit are developed in the framework of a Fourier Grid Hamiltonian method. The aim is to interpret photoassociation experiments in cold atom samples. In order to avoid the implementation of very large grids we propose a mapping procedure adapted to the asymptotic R−n behavior of the long-range potentials. On a single electronic potential, this allows us to determine vibrational wave functions extending up to 500a0 using a minimal number of grid points. Calculations with two electronic states, A 1Σu+ and b 3Πu states, both correlated to the Rb(5s)+Rb(5p) dissociation limit, coupled by fine structure are presented. We predict strong perturbation effects in the Rb2(0u+) spectrum, manifested under the 5s, 5p 2P1/2 dissociation limit by an oscillatory behavior of the rotational constants.
Two identical alkali atoms, with one atom excited, interact at long range through the resonant dipole interaction - C{sub 3}/R{sup 3} and through the dispersion interaction - C{sub 6}/R{sup 6} - C{sub 8}/R{sup 8} - ... These interaction coefficients have been previously calculated, but not accurately measured. The authors have measured the bound levels of a unique, 0{sub g}{sup {minus}}{open_quotes} pure long range state{close_quotes} of {sub 87}Rb{sub 2} and {sup 85}Rb{sub 2} with photoassociation spectroscopy of ultracold Rb atoms. By fitting the levels predicted by the interaction Hamiltonian to the observed levels, they have derived accurate values of both C{sub 3} and of the dispersion interaction coefficients. They also obtain an accurate measurement of the Rb 5s-5p electric dipole matrix element, which is simply related to C{sub 3}. These results provide an excellent test of the theory. They are also important to cold collisions, which are very sensitive to long range interactions.
A reexamination of the photoassociation spectrum of the external well of the ${0}_{g}^{\ensuremath{-}}$ potential of Cs2{\mathrm{Cs}}_{2}Cs2​ converging to the (6s1∕2+6p3∕2)(6{s}_{1∕2}+6{p}_{3∕2})(6s1∕2​+6p3∕2​) limit is performed, in order to resolve inconsistencies arising from a previously published paper [Phys. Rev. Lett. 85, 1408 (2000)]. We use the same analytical description of the potential as in an other previous analysis [Phys. Rev. A 66, 052506 (2002)], but we make a shift of 2 in the assignment of the observed vibrational lines. The agreement between experimental and calculated energy positions is improved and the intensities calculated using the new potential account well for all available data. The fitting procedure reveals a strong interdependence of the parameters of the model, which limits the accuracy of the determination of the radiative lifetimes of the 6p2P1∕26{p}^{2}{P}_{1∕2}6p2P1∕2​ and 6p2P3∕26{p}^{2}{P}_{3∕2}6p2P3∕2​ atomic levels. Only a more precise experimental study could allow one to improve the determination of these lifetime values.
Photoassociation resonances in the 87{}^{87}87Rb2{}_{2}2​ 1g{1}_{g}1g​ state dissociating to 52S+52P1/25{\phantom{\rule{0.16em}{0ex}}}^{2}S+5{}^{2}{P}_{1/2}52S+52P1/2​ were produced by the excitation of colliding 87{}^{87}87Rb atoms in a far-off resonance trap. Levels down to 31 cm${}^{\ensuremath{-}1}$ below the dissociation limit were measured with resonance linewidths of 15 to 20 MHz, and have been located to a one-sigma combined systematic and statistical uncertainty of 50 MHz relative to the 52S+52P1/25{\phantom{\rule{0.16em}{0ex}}}^{2}S+5{}^{2}{P}_{1/2}52S+52P1/2​ limit. Electron and nuclear spins were fixed to a space-fixed axis by circularly polarized optical pumping, so that only states with total nuclear spin I=3I=3I=3 were excited, thereby greatly simplifying the spectrum. The analysis of the data yielded hyperfine coupling parameters A(v)A(v)A(v), vibrational G(v)G(v)G(v), and rotational B(v)B(v)B(v) parameters. The G(v)G(v)G(v) parameters could be fit to an rms accuracy of about 0.01 cm${}^{\ensuremath{-}1}$ to a potential constructed from current C3{C}_{3}C3​ and C6{C}_{6}C6​ long-range dispersion parameters plus an ab initio potential that was adjusted in depth and with quadratic terms in the internuclear distance added to the inner wall.