화학공학소재연구정보센터
Journal of Chemical Physics, Vol.113, No.4, 1524-1534, 2000
van der Waals bending bands of the ArDCN cluster observed by millimeter-wave spectroscopy combined with a pulsed supersonic jet technique
Millimeter-wave absorption spectroscopy combined with a pulsed-jet expansion technique was applied to the measurement of the rovibrational transitions of the van der Waals (vdW) bending bands of the ArDCN cluster in the frequency region of 182 similar to 294 GHz. Sixteen and thirty-seven rovibrational lines were observed for the Sigma(1)-Sigma(0) and Pi(1)-Sigma(0) bands, respectively, split into hyperfine structure due to the nitrogen nucleus. A set of accurate molecular constants, including the band origins, rotational constants, nuclear quadrupole coupling constants, and the Coriolis interaction constant between the Sigma(1) and Pi(1) bending substates, was determined. The band origins for the Sigma(1)-Sigma(0) and Pi(1)-Sigma(0) bands of ArDCN, 189.017 380(7) GHz and 195.550 736(12) GHz, are larger by 24.126 585(9) and 13.566 314(16) GHz than the corresponding values of ArHCN, respectively. The abnormal isotopic effect on the vibrational frequencies is attributed to the characteristic potential energy surface of ArH(D)CN, which has two minima, corresponding to the linear configuration and a much shallower minimum at the T-shaped configuration. The rotational and quadrupole coupling constants for the excited states are quite different from those of the ground state. For example, the rotational constants 1926.8863(16) and 1967.8768(9) MHz for the excited Sigma(1) and Pi(1) states are significantly larger than that of the ground Sigma(0) state, 1574.793 16(24) MHz. It indicates the shrinkage of the bond length of the cluster by about 0.402 similar to 0.440 Angstrom on the excitation of the vdW bending mode, together with the change from the linear form in the ground (j = 0) state to the T-shaped form in the first excited (j = 1) state. The determined molecular constants were compared with those calculated with the potential energy surface calculated at CCSD(T) level.