Abstract

Experimentally and theoretically determined magnetic and electric dipole moments, bond distances, and vibrational spacings are used for a comparative study of the bonding in ThF and ThCl. Numerous bands in the visible electronic spectra between 16 400 and 18 800 cm-1 of supersonically cooled molecular beam samples have been detected using medium-resolution (Δν ≈ 0.1 cm-1) 2D spectroscopy. High-resolution (Δν < 20 MHz) field-free, Stark, and Zeeman spectroscopy of the detected [18.6]Ω = 3/2 - X2Δ3/2 band of ThF near 538.4 nm and the [18.2]Ω = 3/2 - X2Δ3/2 band of ThCl near 551.0 nm have been recorded and analyzed. Stark shifts and splitting were analyzed to produce | μ⃗el| values of 1.453(7) D and 0.588(9) D for the X2Δ3/2 and [18.6]Ω = 3/2 states of ThF, respectively, and 2.022(35) D and 3.020(55) D for the X2Δ3/2 and [18.2]Ω = 3/2 states of ThCl. Zeeman splittings and shifts were analyzed to produce ge values of 1.038(4) and 1.079(4) for the X2Δ3/2 and [18.6]Ω = 3/2 states of ThF and 1.130(4) and 1.638(4) for the X2Δ3/2and [18.2]Ω = 3/2 states of ThCl. Analysis of ge values demonstrates that the X2Δ3/2 and [18.6]Ω = 3/2 states of ThF and the X2Δ3/2 state of ThCl are predominately 2Δ3/2 spin-orbit components, whereas the [18.2]Ω = 3/2 state of ThCl is an admixture of 2Δ3/2 and 2Π3/2 spin-orbit components. A molecular orbital description of the ground states is used to rationalize the observed | μ⃗el|values for the ThX (X = F, Cl, O, and S) series and garner insight into the bonding mechanism. The dipole moments in the ground state of ThF and ThCl have been calculated using relativistic coupled-cluster methods. It is demonstrated that the systematic inclusion of electron-correlation contributions plays an essential role in obtaining accurate predictions for the dipole-moment values in ThF and ThCl.

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