Experimental dipole moment function and calculated radiative lifetimes for vibrational transitions in carbon monoxide a 3Π

1975 ◽  
Vol 63 (9) ◽  
pp. 3756 ◽  
Author(s):  
Brian G. Wicke ◽  
William Klemperer
1984 ◽  
Vol 62 (12) ◽  
pp. 1579-1585 ◽  
Author(s):  
C. Chackerian Jr. ◽  
R. Farrenq ◽  
G. Guelachvili ◽  
C. Rossetti ◽  
W. Urban

Experimental intensity information is combined with numerically obtained vibrational wave functions in a nonlinear least-squares fitting procedure to obtain the ground electronic state electric dipole moment function of carbon monoxide valid in the range of nuclear oscillation (0.87–1.91 Å) of about the V = 38th vibrational level. Vibrational transition matrix elements are computed from this function for ΔV = 1, 2, 3 with V ≤ 38.


1978 ◽  
Vol 56 (6) ◽  
pp. 727-736 ◽  
Author(s):  
P. Niay ◽  
P. Bernage ◽  
C. Coquant ◽  
R. Houdart

By using a SISAM spectrometer with a 0.03 cm−1 resolving power we have measured the line-strengths for the 4 ← 0 and 5 ← 0 absorption bands of the HI molecule. The pressure in the White cell was important enough to assume the lines to be described through a Lorentz profile, and we have used the 'curve of growth' method. By using all the available data on the 1 ← 0,2 ← 0, and 3 ← 0 bands, we have calculated the first six coefficients of the dipole moment expansion series. The shape of the experimental dipole moment function shows that the HI bond is primarily covalent.


1957 ◽  
Vol 26 (6) ◽  
pp. 1671-1677 ◽  
Author(s):  
William S. Benedict ◽  
Robert Herman ◽  
Gordon E. Moore ◽  
Shirleigh Silverman

1981 ◽  
Vol 44 (1) ◽  
pp. 111-123 ◽  
Author(s):  
Hans-Joachim Werner

1977 ◽  
Vol 32 (8) ◽  
pp. 897-898 ◽  
Author(s):  
Y. K. Chan ◽  
B. S. Rao

Abstract The radial Schrödinger wave equation with Morse potential function is solved for HF molecule. The resulting vibration-rotation eigenfunctions are then used to compute the matrix elements of (r - re)n. These are combined with the experimental values of the electric dipole matrix elements to calculate the dipole moment coefficients, M 1 and M 2.


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