The permanent electric dipole moments of the ground, and the low-lying excited electronic states of platinum monocarbide, PtC, platinum monoxide, PtO, and platinum monosulfide, PtS, were measured using a molecular beam optical Stark spectroscopic scheme. The determined values were (in Debye): PtO(X 3Σ−) 2.77(2); PtO(A 1Σ+) 1.15(4); PtS[X(Ω=0)] 1.78(2); PtS[B(Ω=0)] 0.54(6); PtC(X 1Σ+) 0.99(5); and PtC(A 1Π) 2.454(3). These results, along with the previous results for PtN(X 2Π1/2) 1.977(9); PtN(d 4Π1/2) 1.05(9) [J. Chem. Phys. 102, 643 (1995)], are used as a basis for a discussion of the nature of the electronic states.

The gaseous products generated in the supersonic coexpansion of laser ablated platinum vapor with methane or acetylene were probed by visible laser induced fluorescence (LIF) spectroscopy. Both platinum monocarbide, PtC, and an unidentified Pt-containing polyatomic molecule were detected. The intense (0,0)A′ 1Π→X 1Σ+ (T00=13 196.13 cm−1) and (0,0)A 1Π→X 1Σ+ (T00=18 510.71 cm−1) band systems of PtC were recorded at a resolution of ∼0.001 cm−1. The magnetic hyperfine splitting exhibited in the spectral features of the 195PtC isotopomer was analyzed and indicates that the A′ 1Π and A 1Π states arise primarily from a...σ1π1 and a...δ3π1 configurations, respectively.

No abstract