“…A representation of the apparatus is shown in [22]. The experimental setup used here was similar to the one used previously for Rb 2 [48].…”
Section: Fluorescence From Higher-lying Statesmentioning
confidence: 99%
“…There have also been a succession of studies of the A and b states of the lighter homonuclear alkali dimer species Li 2 [33][34][35][36], Na 2 [22,[37][38][39][40][41], K 2 [18,20,[42][43][44][45][46] and Rb 2 [47,48]. For Na 2 [22], data now extend almost continuously from the lowest vibrational levels to the atomic limit.…”
We present experimentally derived potential curves and spin-orbit interaction functions for the strongly perturbed A 1 Σ + u and b 3 Πu states of the cesium dimer. The results are based on data from several sources. Laser-induced fluorescence Fourier transform spectroscopy (LIF FTS) was used some time ago in the Laboratoire Aimé Cotton primarily to study the X 1 Σ + g state. More recent work at Tsinghua University provides information from moderate resolution spectroscopy on the lowest levels of the b 3 Π ± 0u states as well as additional high resolution data. From Innsbruck University, we have precision data obtained with cold Cs2 molecules. Recent data from Temple University was obtained using the optical-optical double resonance polarization spectroscopy technique, and finally, a group at the University of Latvia has added additional LIF FTS data. In the Hamiltonian matrix, we have used analytic potentials (the Expanded Morse Oscillator form) with both finite-difference (FD) coupled-channels and discrete variable representation (DVR) calculations of the term values. Fitted diagonal and off-diagonal spin-orbit functions are obtained and compared with ab initio results from Temple and Moscow State universities.
“…A representation of the apparatus is shown in [22]. The experimental setup used here was similar to the one used previously for Rb 2 [48].…”
Section: Fluorescence From Higher-lying Statesmentioning
confidence: 99%
“…There have also been a succession of studies of the A and b states of the lighter homonuclear alkali dimer species Li 2 [33][34][35][36], Na 2 [22,[37][38][39][40][41], K 2 [18,20,[42][43][44][45][46] and Rb 2 [47,48]. For Na 2 [22], data now extend almost continuously from the lowest vibrational levels to the atomic limit.…”
We present experimentally derived potential curves and spin-orbit interaction functions for the strongly perturbed A 1 Σ + u and b 3 Πu states of the cesium dimer. The results are based on data from several sources. Laser-induced fluorescence Fourier transform spectroscopy (LIF FTS) was used some time ago in the Laboratoire Aimé Cotton primarily to study the X 1 Σ + g state. More recent work at Tsinghua University provides information from moderate resolution spectroscopy on the lowest levels of the b 3 Π ± 0u states as well as additional high resolution data. From Innsbruck University, we have precision data obtained with cold Cs2 molecules. Recent data from Temple University was obtained using the optical-optical double resonance polarization spectroscopy technique, and finally, a group at the University of Latvia has added additional LIF FTS data. In the Hamiltonian matrix, we have used analytic potentials (the Expanded Morse Oscillator form) with both finite-difference (FD) coupled-channels and discrete variable representation (DVR) calculations of the term values. Fitted diagonal and off-diagonal spin-orbit functions are obtained and compared with ab initio results from Temple and Moscow State universities.
“…First studies of such kind of system have been reported for the Rb-containing alkali diatomics, in which apparent disorder in vibrational spacing was observed for Rb 2 [17], see [18] for more extensive studies, NaRb [19] and RbCs [20]. The crucial issue however remained unsolved, namely, while the experimental term values were obtained with high precision of about 0.003-0.01 cm −1 , the resulting deperturbed parameters reproduced experimental data with much poorer accuracy of 0.05-0.25 cm −1 [18,19,20]. Furthermore, even the vibrational numbering of the "dark" triplet b 3 Π state was still remained questionable.…”
The laser induced fluorescence (LIF) spectra A 1 Σ + ∼ b 3 Π(E J ) → X 1 Σ + of KCs dimer were recorded in near infrared region by Fourier Transform Spectrometer with a resolution of 0.03 cm −1 . Overall more than 200 collisionally enhanced LIF spectra were rotationally assigned to 39 K 133 Cs and 41 K 133 Cs isotopomers yielding with the uncertainty of 0.003-0.01 cm −1 more than 3400 rovibronic term values of the strongly mixed singlet A 1 Σ + and triplet b 3 Π states. Experimental data massive starts from the lowest vibrational level vA = 0 of the singlet and nonuniformly cover the energy range E J ∈ [10040, 13250] cm −1 with rotational quantum numbers J ∈ [7, 225]. Besides of the dominating regular A 1 Σ + ∼ b 3 ΠΩ=0 interactions the weak and local heterogenous A 1 Σ + ∼ b 3 ΠΩ=1 perturbations have been discovered and analyzed. Coupled-channel deperturbation analysis of the experimental 39 K 133 Cs e-parity termvalues of the A 1 Σ + ∼ b 3 ΠΩ=0,1,2 complex was accomplished in the framework of the phenomenological 4 × 4 Hamiltonian accounting implicitly for regular interactions with the remote 1 Π and 3 Σ + states manifold. The resulting diabatic potential energy curves of the interacting states and relevant spin-orbit coupling matrix elements defined analytically by Expanded Morse Oscillators model reproduce 95% of experimental data field of the 39 K 133 Cs isotopomer with a standard deviation of 0.004 cm −1 which is consistent with the uncertainty of the experiment. Reliability of the derived parameters was additionally confirmed by a good agreement between the predicted and experimental termvalues of 41 K 133 Cs isotopomer. Calculated relative intensity distributions in the A ∼ b → X LIF progressions are also consistent with their experimental counterparts. Finally, the deperturbation model was applied for a simulation of pump-dump optical cycle a 3 Σ + → A 1 Σ + ∼ b 3 Π → X 1 Σ + proposed for transformation of ultracold colliding K+Cs pairs to their ground molecular state vX = 0; JX = 0.
“…It would represent a test of the spin-orbit coupling used in the calculation. In this respect, a new perspective for the present analysis is offered by the recent determination of the potential curves and spin-orbit coupling of the (A, b) coupled system in Rb 2 , extracted from the compilation of several high-resolution spectroscopic data [19]. Indeed, the present calculations could be run again with these new accurate data, in order to predict the predissociation width over the whole energy range between P 1/2 and P 3/2 , and [28], below the P 1/2 asymptote taken as the origin of energies.…”
Section: Discussionmentioning
confidence: 99%
“…This is particularly true in heavy alkali dimers like Rb 2 [18,19], which required novel methods to deperturb the spectra recorded in high-resolution molecular spectroscopic studies [20,21], where almost all rovibrational levels exhibit a mixed singlet/triplet character up to the dissociation limits. This pattern has also been observed in heteronuclear systems involving one heavy alkali atom like NaRb [22,23], NaCs [24], and RbCs [25].…”
Section: The (A B) Coupled State System In the Rubidium Dimermentioning
This work stresses the importance of the choice of the set of reference functions in the Generalized Multichannel Quantum Defect Theory to analyze the location and the width of Feshbach resonance occurring in collisional cross-sections. This is illustrated on the photoassociation of cold rubidium atom pairs, which is also modeled using the Mapped Fourier Grid Hamiltonian method combined with an optical potential. The specificity of the present example lies in a high density of quasi-bound states (closed channel) interacting with a dissociation continuum (open channel). We demonstrate that the optimization of the reference functions leads to quantum defects with a weak energy dependence across the relevant energy threshold. The main result of our paper is that the agreement between the both theoretical approaches is achieved only if optimized reference functions are used.
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