Abstract

High resolution spectra of the B 1Π←X 1Σ+ transition of the 39K85Rb molecule have been measured with the technique of Doppler-free optical–optical double resonance polarization spectroscopy. Molecular constants of the B 1Π(v′=0−12) levels are determined, and the RKR potential is calculated. A number of irregularities in the energies of B 1Π state levels and intensity anomalies are observed. The energy shifts of the e and f levels of the B 1Π state are studied, and the perturbations between the B 1Π and 3Σ+ states and between the B 1Π and 3Π1 states are identified. Several transitions to the 3Π1 and 3Σ+ states are also observed, and the molecular constants of the 3Π1 and 3Σ+ states are evaluated. The single rovibrational level B 1Π(v′=2, J′=41) is selectively excited by a single frequency laser chopped by an electro-optical modulator, and the decay time of the resulting fluorescence is measured at various pressures. From the Stern–Volmer plot, the radiative lifetime and the collisional cross section of the fluorescence quenching are determined to be 11.6 ns and 29 Å2, respectively. The intensity distribution of the dispersed fluorescence of the B 1Π(v′=2, J′=41)→X 1Σ+(v″=0−11, J″=42) transitions is in very good agreement with the calculated values of ν4|〈v′=2|v″〉|2. The magnitude of the transition dipole moment is determined to be 9.2 D in the range of 4.08 Å<R<4.73 Å. These results are compared with the results of recent ab initio calculations.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.