DIRECT OBSERVATION OF THE 2 $^{3}\Pi_{u}$ STATE OF $Rb_{2}$ IN A PULSED MOLECULAR BEAM: ROTATIONAL-BRANCH INTENSITY ANOMALIES IN THE 2 $^{3}\Pi_{u}(1_{u}) - X^{1}\Sigma^{+}_{g}(0^{+}_{g})$ BANDS

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2000

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Ohio State University

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The first observation of 2 3ΠuX1Σg+ transitions is reported. Rotationally resolved transitions of the 2 3Πu(1u)X1Σg+(0g+) and 2 3Πu(0u+)−X1Σg+(0g+) are observed by resonance enhanced 2-photon ionization (RE2PI) method in a pulsed molecular beam. Ω-doubling and interference induced rotational branch intensity anomalies are observed for 2 3Πu(1u)−X1Σg+(0g+) transitions. Both of 2 3Πu(0u+) and 2 3Πu(1u) states are strongly mixed with singlet slates by spin-orbit coupling. The former with 2 1Σu+ and the latter with 2 1Πu. In relatively weak 2 3Πu(1u) bands P-branch rotational lines disappear and the intensities of R-branch rotational lines are enhanced. These intensity anomalies in 2 3Πu(1u)−X1Σg+(0g+) transition, due to an interference effect between parallel and perpendicular transition amplitudes, is caused by ΔΩ=±1 perturbation. The molecular constants of 2 3Πu(0u+)−X1Σg+(0g+) transition are determined as Tc=19784.2588±0.0088cm−1,ωe=42.1954±0.0060cm−1,ωexe=0.1701±0.0011cm−1,ωeye=−0.001096±0.000057cm−1,Be=0.018603±0.000018cm−1 for 85Rb2. The spin-orbit coupling constant A and Ω-doubling parameters p and q are determined by simultaneous fitting of the rotational contours of both 2 3Πu(1u)−X1(Σg+) and 2 3Πu(0u+)−X1Σg+(0g+) transitions.

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Author Institution: Department of Chemistry, Korea Advanced Institute of Science and Technology

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