The PF2(H 4A1) radical has been generated by flowing PFS through a dc discharge using He or Ar carrier gas. The PF# 'A\*-% 'B, ) low-resolution emission spectrum has been analyzed to obtain v,,, o; , w; and some anharmonic constants. The radiative lifetime of the PF,( 8 'AZ) state is > 1.9 ms.
Improvement of the Spectroscopic Constants of the PF(A3Π) State and Assignment of the PF(A–X) Transition Dipole Function
✍ Scribed by B. Nizamov; D.W. Setser
- Publisher
- Elsevier Science
- Year
- 2001
- Tongue
- English
- Weight
- 236 KB
- Volume
- 206
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
High-resolution laser-excitation spectra were acquired for the v = 3-7 levels of the PF(A 3 0,1,2 ← X 3 -) transition from PF(X 3 -) molecules generated in a discharge flow reactor. These results were combined with lower resolution excitation spectra for the v = 8-11 levels and with existing high-resolution data in the literature for v = 0 and 1 to assign improved spectroscopic constants for PF(A 3 0,1,2 ). The abnormal vibrational energy level spacings for all spin components of the PF(A 3 ) state are evidence for a homogeneous interaction with another 3 state. The -doublet separation in the PF( 3 0 ) substate increases with vibrational level, which is taken as evidence for interaction with the PF(b 1 + ) state. Laser-induced fluorescence spectra from individual v = 0-5 levels were used to obtain vibrational band intensities of the A-X transition. The strong dependence of the transition dipole on the r-centroid is consistent with the reduction in the radiative lifetimes with increasing v level. The similarity between the isovalent PF(A 3 ) and SO(A 3 ) states is noted and the bond dissociation energy of PF(X 3 -) is discussed.
📜 SIMILAR VOLUMES
The potential energy curves, dipole, quadrupole and octopole moments and dipole polarisabilities have been calculated at CASSCF level using a [ 8s6p3d] basis for the ground X 2~ + state of CO + as a function of internuclear distance. In addition the potential energy curves, as well as the dipole, qu