Infrared spectra of PD3 have been recorded in the 600-1160 cm-1 range at a resolution of 0.0023 cm-1. About 2500 rovibrational transitions have been measured and assigned to the v2(A1) and v4(E) bending fundamentals, including 131 "perturbation allowed" transitions with selection rules Δ(k-1) = ±3 and ±6. Splittings of the K″ = 3, 6, and 9 lines were observed. The rotational structure in the v2 = 1 and v4 = 1 vibrational states up to J = K = 28 was reproduced by fitting simultaneously all experimental data. The adopted rovibrational Hamiltonian explicitly takes into account the Coriolis and k-type interactions between the v2 = 1 and v4 = 1 states, and includes also several essential resonances within these states. Two different reductions of the Hamiltonian were adopted in the fitting procedure. The 41 parameters in model 1 reproduced 2435 IR transitions retained in the final cycle with a standard deviation of the fit equal to 2.06 × 10-4 cm-1 (about the precision of experimental measurements); in model 2, 45 parameters reproduced 2428 transitions with the same value of standard deviation. The equivalence of the two sets of parameters has been demonstrated.
Cane' E., Fusina L., Jerzembeck W., Burger H. (2003). The v2 and v4 bending fundamental bands of PD3. JOURNAL OF MOLECULAR SPECTROSCOPY, 218(1), 28-35 [10.1016/S0022-2852(02)00026-7].
The v2 and v4 bending fundamental bands of PD3
Cane' E.Primo
;Fusina L.
Secondo
;
2003
Abstract
Infrared spectra of PD3 have been recorded in the 600-1160 cm-1 range at a resolution of 0.0023 cm-1. About 2500 rovibrational transitions have been measured and assigned to the v2(A1) and v4(E) bending fundamentals, including 131 "perturbation allowed" transitions with selection rules Δ(k-1) = ±3 and ±6. Splittings of the K″ = 3, 6, and 9 lines were observed. The rotational structure in the v2 = 1 and v4 = 1 vibrational states up to J = K = 28 was reproduced by fitting simultaneously all experimental data. The adopted rovibrational Hamiltonian explicitly takes into account the Coriolis and k-type interactions between the v2 = 1 and v4 = 1 states, and includes also several essential resonances within these states. Two different reductions of the Hamiltonian were adopted in the fitting procedure. The 41 parameters in model 1 reproduced 2435 IR transitions retained in the final cycle with a standard deviation of the fit equal to 2.06 × 10-4 cm-1 (about the precision of experimental measurements); in model 2, 45 parameters reproduced 2428 transitions with the same value of standard deviation. The equivalence of the two sets of parameters has been demonstrated.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.