Journal of Molecular Spectroscopy -- June 1995 -- vol.171, no.2, pp. 420-34 Intensities of hot-band transitions: HCN hot bands Maki, A.; Quapp, W.; Klee, S. A simple vibrational Honl-London-type formula for hot-band intensities is tested by measuring the intensities of a number of vibrational transitions, including many hot bands, for HCN. This vibrational intensity formula is based on one- and two-dimensional harmonic oscillator functions and a nonlinear electric dipole function that is expanded in a Taylor series with respect to the normal coordinates. It is shown that, when this formula is included, the observed transition dipoles for the bending hot bands differ by only a few percent from the transition dipoles for the same quantum number changes from the ground state. Infrared absorption intensity measurements are given for the transition dipoles for the transitions 01^1/0-00^0/0, 02^0/0-00^0/0, 03^1/0-00^0/0, 04^0/0-00^0/0, 10^0/0-01^1/0, 12^0/0-00^0/0, and 20^0/0-00^0/0 and the accompanying hot bands involving the lower states v_2 =1, 2, and 3. This simple model is limited to well-behaved systems, but would be useful for estimating the intensities of some high-temperature spectra. For HCN the Herman-Wallis constants that are quadratic in J (or m) are shown to be determined principally by the effect of l-type resonance Doc. Type Journal Paper; Theoretical or Mathematical; Experimental Coden JMOSA3 ISSN 0022-2852 Classification codes A3320E; A3310G; A3520P; A3370F Indexing: hydrogen compounds; infrared spectra; spectral line intensity; vibrational states; hot band transitions; HCN; vibrational Honl-London-type formula; hot-band intensities; vibrational transitions; room temperature spectrum; vibrational intensity formula; one-dimensional harmonic oscillator functions; two-dimensional harmonic oscillator functions; Taylor series; nonlinear electric dipole function; normal coordinates; transition dipoles; bending hot bands; quantum number changes; ground state; IR absorption intensity; well-behaved systems; Herman-Wallis constants