Abstract:Van der Waals coefficients for the heteronuclear alkali-metal dimers of Li, Na, K, Rb, Cs, and Fr are calculated using relativistic ab initio methods augmented by high-precision experimental data. We argue that the uncertainties in the coefficients are unlikely to exceed about 1%.
“…The scattering lengths found are consistent with previous determinations [16,22]. Our C 6 coefficient agrees with the values found in ab initio calculations [14,23].…”
Section: Formation Of Fermionic Molecules Via Interisotope Feshbach Rsupporting
We perform an analysis of recent experimental measurements and improve the lithium interaction potentials. For 6 Li a consistent description can be given. We discuss theoretical uncertainties for the position of the wide 6 Li Feshbach resonance, and we present an analytic scattering model for this resonance, based on the inclusion of a field-dependent virtual open-channel state. We predict new Feshbach resonances for the 6 Li-7 Li system, and their importance for different types of crossover superfluidity models is discussed.
“…The scattering lengths found are consistent with previous determinations [16,22]. Our C 6 coefficient agrees with the values found in ab initio calculations [14,23].…”
Section: Formation Of Fermionic Molecules Via Interisotope Feshbach Rsupporting
We perform an analysis of recent experimental measurements and improve the lithium interaction potentials. For 6 Li a consistent description can be given. We discuss theoretical uncertainties for the position of the wide 6 Li Feshbach resonance, and we present an analytic scattering model for this resonance, based on the inclusion of a field-dependent virtual open-channel state. We predict new Feshbach resonances for the 6 Li-7 Li system, and their importance for different types of crossover superfluidity models is discussed.
“…The dispersion coefficients C 6 and C 8 are taken from Refs. [40,41]. With the present data sets we are also able to reproduce the experimental data with the same quality of the fit by fixing these coefficients to the values from Ref.…”
Section: Construction Of Potential Energy Curvesmentioning
confidence: 58%
“…R o is chosen as described in Refs. [27,38], the C 6 and C 8 coefficients are fixed to their theoretical values [39,40,41], γ and β are estimated using the ionization potentials for Li and Cs [42] according to Ref. [37], while U ∞ , C 10 and A ex are adjusted during the fitting procedure.…”
Section: Construction Of Potential Energy Curvesmentioning
We present the first high-resolution spectroscopic study of LiCs. LiCs is formed in a heat pipe oven and studied via laser-induced fluorescence Fourier-transform spectroscopy. By exciting molecules through the X 1 Σ + -B 1 Π and X 1 Σ + -D 1 Π transitions vibrational levels of the X 1 Σ + ground state have been observed up to 3 cm −1 below the dissociation limit enabling an accurate construction of the potential. Furthermore, rovibrational levels in the a 3 Σ + triplet ground state have been observed because the excited states obtain sufficient triplet character at the corresponding excited atomic asymptote. With the help of coupled channels calculations accurate singlet and triplet ground state potentials were derived reaching the atomic ground state asymptote and allowing first predictions of cold collision properties of Li + Cs pairs.
“…The energy of these states is obtained by finding the poles of the total S matrix Eq. (22). This results in solving we readily obtain…”
Section: B Tailored Feshbach Theorymentioning
confidence: 97%
“…(17). The van der Waals coefficient used is C 6 = 2322E h a 6 0 [22], where E h = 4.359 74 × 10 −18 J and a 0 = 0.052 917 72 nm. The value of η 01 11 has been plotted as a function of the triplet binding energy 1 for three different values of the singlet binding energy 0 .…”
We present an asymptotic-bound-state model which can be used to accurately describe all Feshbach resonance positions and widths in a two-body system. With this model we determine the coupled bound states of a particular two-body system. The model is based on analytic properties of the two-body Hamiltonian and on asymptotic properties of uncoupled bound states in the interaction potentials. In its most simple version, the only necessary parameters are the least bound state energies and actual potentials are not used. The complexity of the model can be stepwise increased by introducing threshold effects, multiple vibrational levels, and additional potential parameters. The model is extensively tested on the 6 Li-40 K system and additional calculations on the 40 K-87 Rb system are presented.
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