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Physical Review A

Potentials for modeling cold collisions between Na (3S) and Rb (5S) atoms

A. Pashov, O. Docenko, M. Tamanis, R. Ferber, H. Knöckel, E. Tiemann

Published Dec 21, 2005• 77 citations
Publisher

Abstract

The experimental characterization of the electronic states correlated to the asymptote of ground state Na (3S) and Rb (5S) atoms was expanded by spectroscopic data on $a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}$ state levels using a high resolution Fourier transform spectroscopy technique. The hyperfine splitting of the $a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}$ state levels was partially resolved and analyzed for both $\mathrm{Na}\phantom{\rule{0.2em}{0ex}}^{85}\mathrm{Rb}$ and $\mathrm{Na}\phantom{\rule{0.2em}{0ex}}^{87}\mathrm{Rb}$ isotopomers. Transitions to high lying levels of the $a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}$ and $X\phantom{\rule{0.2em}{0ex}}^{1}\ensuremath{\Sigma}^{+}$ states were recorded simultaneously which enables one to determine long range parameters of the molecular potentials. Coupled channels calculations based on the Fourier grid method were finally applied for deriving accurate potential energy curves of the $a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}$ and $X\phantom{\rule{0.2em}{0ex}}^{1}\ensuremath{\Sigma}^{+}$ states capable of a reliable description of cold collisions between Na and Rb atoms in their ground states. Scattering lengths and Feshbach resonances were calculated for some quantum states.

DOI
10.1103/physreva.72.062505

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We observe bound states just below the dissociation limit and shape and Feshbach resonances between the ground state hyperfine asymptotes by Raman spectroscopy on a molecular beam of sodium dimers. The rotational selectivity of a two-photon transition gives access to specific states of nuclear motion and thus to cold collision properties of two colliding atoms. Modeling of the collisional resonance structures requires a multichannel treatment of the nuclear dynamics that uses highly accurate $X{}^{1}{\ensuremath{\Sigma}}_{g}^{+}$ and $a{}^{3}{\ensuremath{\Sigma}}_{u}^{+}$ potentials. These potentials are constructed from bound levels just below the ground state asymptote measured in this experiment and bound state information available in the literature. We also present simulations of the spectrum between the ground state hyperfine asymptotes. The good agreement shows that accurate potentials obtained from bound state information are able to reproduce scattering properties of two colliding sodium atoms. From this analysis we find for the scattering lengths ${a(f=2)=a}_{1,\ensuremath{-}1}{=52.98(40)a}_{0},$ ${a}_{\mathrm{singlet}}{=19.20(30)a}_{0},$ and ${a}_{\mathrm{triplet}}{=62.51(50)a}_{0},$ where ${1a}_{0}=0.0529177$ nm.

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The experimental characterization of the electronic states correlated to the asymptote of ground state Na (3S) and Rb (5S) atoms was expanded by spectroscopic data on a3\ensuremathΣ+a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}a3\ensuremathΣ+ state levels using a high resolution Fourier transform spectroscopy technique. The hyperfine splitting of the a3\ensuremathΣ+a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}a3\ensuremathΣ+ state levels was partially resolved and analyzed for both Na85Rb\mathrm{Na}\phantom{\rule{0.2em}{0ex}}^{85}\mathrm{Rb}Na85Rb and Na87Rb\mathrm{Na}\phantom{\rule{0.2em}{0ex}}^{87}\mathrm{Rb}Na87Rb isotopomers. Transitions to high lying levels of the a3\ensuremathΣ+a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}a3\ensuremathΣ+ and X1\ensuremathΣ+X\phantom{\rule{0.2em}{0ex}}^{1}\ensuremath{\Sigma}^{+}X1\ensuremathΣ+ states were recorded simultaneously which enables one to determine long range parameters of the molecular potentials. Coupled channels calculations based on the Fourier grid method were finally applied for deriving accurate potential energy curves of the a3\ensuremathΣ+a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}a3\ensuremathΣ+ and X1\ensuremathΣ+X\phantom{\rule{0.2em}{0ex}}^{1}\ensuremath{\Sigma}^{+}X1\ensuremathΣ+ states capable of a reliable description of cold collisions between Na and Rb atoms in their ground states. Scattering lengths and Feshbach resonances were calculated for some quantum states.
The states X 1 Σ + and a 3 Σ + correlated to the ground-state asymptote of Na (3s) and Cs (6s) atoms have been experimentally investigated using high resolution Fourier-transform spectroscopy. The hyperfine splitting of the a 3 Σ + state levels is partially resolved. Transitions to asymptotic vibrational levels of the a 3 Σ + and X 1 Σ + states were recorded simultaneously. The joint evaluation of the data of both the a 3 Σ + and the X 1 Σ + states allows us to determine accurate potential energy curves of both electronic states. Coupled-channels calculations are finally applied for deriving long range dispersion parameters and the exchange contribution of the molecular potentials, yielding a reliable description of cold collisions between Na and Cs atoms in their two different hyperfine ground states. Scattering lengths and Feshbach resonances are predicted for selected quantum states.
A comprehensive study of the electronic states at the 4s+5s4s+5s4s+5s asymptote in KRb\mathrm{KRb}KRb is presented. Abundant spectroscopic data on the $a\phantom{\rule{0.2em}{0ex}}^{3}\ensuremath{\Sigma}^{+}$ state were collected by Fourier-transform spectroscopy, which allows one to determine an accurate experimental potential energy curve up to 14.8A˚14.8\phantom{\rule{0.3em}{0ex}}\mathrm{\AA{}}14.8A˚. The existing data set [C. Amiot et al., J. Chem. Phys. 112, 7068 (2000)] on the ground state $X\phantom{\rule{0.2em}{0ex}}^{1}\ensuremath{\Sigma}^{+}$ was extended by several additional levels lying close to the atomic asymptote. In a coupled channels fitting routine complete molecular potentials for both electronic states were fitted. Along with the line frequencies of the molecular transitions, recently published positions of Feshbach resonances in 40K^{40}\mathrm{K}40K and 87Rb^{87}\mathrm{Rb}87Rb mixtures [F. Ferlaino et al., Phys. Rev. A 74, 039903 (2006)] were included in the fit. This makes the derived potential curves capable for an accurate description of observed cold collision features so far. Predictions of scattering lengths and Feshbach resonances in other isotopic combinations are reported.
A comprehensive study of the $X\text{ }{^{1}\ensuremath{\Sigma}}^{+}$ and $a\text{ }{^{3}\ensuremath{\Sigma}}^{+}$ electronic states of the K and Cs atom pair is presented. Abundant spectroscopic data include 1937 transitions to the $a\text{ }{^{3}\ensuremath{\Sigma}}^{+}$ state and 13 72413\text{ }72413 724 transitions to the $X\text{ }{^{1}\ensuremath{\Sigma}}^{+}$ state for 39K 133Cs{^{39}\text{K}\text{ }}^{133}\text{Cs}39K 133Cs which were obtained by Fourier-transform spectroscopy. From these data potential energy curves were constructed simultaneously for both states $X\text{ }{^{1}\ensuremath{\Sigma}}^{+}$ and $a\text{ }{^{3}\ensuremath{\Sigma}}^{+}$ which are coupled by the hyperfine interaction. This allows us to accurately model the potential close to K(4s)+Cs(6s)\text{K}(4s)+\text{Cs}(6s)K(4s)+Cs(6s) atom-pair asymptote which is required to simulate cold collision processes. Dissociation energies of the $X\text{ }{^{1}\ensuremath{\Sigma}}^{+}$ state as ${D}_{e}^{X}=4069.208(40)\text{ }{\text{cm}}^{\ensuremath{-}1}$ and of the $a\text{ }{^{3}\ensuremath{\Sigma}}^{+}$ state as ${D}_{e}^{a}=267.141(20)\text{ }{\text{cm}}^{\ensuremath{-}1}$ were determined. Scattering lengths are predicted for different KCs isotopologs and Feshbach resonances were calculated for magnetic fields up to 1000 G.
We review the information on the interactions between cold ground-state Na atoms following from Na2{\mathrm{Na}}_{2}Na2​ bound states, a Na photoassociation experiment, and a recent observation of field-induced Feshbach resonances in a Na Bose condensate. We obtain a set of Na interaction parameters that is in excellent agreement with all these experimental data. The existing discrepancy between different values for the scattering length ${a}_{1,\ensuremath{-}1}$ of Na atoms in the $|1,\ensuremath{-}1〉$ hyperfine state is resolved. The present interaction parameters enable us to give accurate predictions for the singlet and triplet scattering lengths aS{a}_{S}aS​ and aT,{a}_{T},aT​, ${a}_{1,\ensuremath{-}1},$ scattering lengths for collisions between Na atoms in other hyperfine states, and resonance fields of several yet unobserved Feshbach resonances. We find ${a}_{S}=(19.1\ifmmode\pm\else\textpm\fi{}{2.1)a}_{0},{a}_{T}=(65.3\ifmmode\pm\else\textpm\fi{}{0.9)a}_{0},$ and ${a}_{1,\ensuremath{-}1}(B=0)=(55.4\ifmmode\pm\else\textpm\fi{}{1.2)a}_{0}.$
We observe bound states just below the dissociation limit and shape and Feshbach resonances between the ground state hyperfine asymptotes by Raman spectroscopy on a molecular beam of sodium dimers. The rotational selectivity of a two-photon transition gives access to specific states of nuclear motion and thus to cold collision properties of two colliding atoms. Modeling of the collisional resonance structures requires a multichannel treatment of the nuclear dynamics that uses highly accurate $X{}^{1}{\ensuremath{\Sigma}}_{g}^{+}$ and $a{}^{3}{\ensuremath{\Sigma}}_{u}^{+}$ potentials. These potentials are constructed from bound levels just below the ground state asymptote measured in this experiment and bound state information available in the literature. We also present simulations of the spectrum between the ground state hyperfine asymptotes. The good agreement shows that accurate potentials obtained from bound state information are able to reproduce scattering properties of two colliding sodium atoms. From this analysis we find for the scattering lengths ${a(f=2)=a}_{1,\ensuremath{-}1}{=52.98(40)a}_{0},$ asinglet=19.20(30)a0,{a}_{\mathrm{singlet}}{=19.20(30)a}_{0},asinglet​=19.20(30)a0​, and atriplet=62.51(50)a0,{a}_{\mathrm{triplet}}{=62.51(50)a}_{0},atriplet​=62.51(50)a0​, where 1a0=0.0529177{1a}_{0}=0.05291771a0​=0.0529177 nm.