Diatom potential curves and transition moment functions from continuum absorption coefficients: Br2
- 15 August 1976
- journal article
- research article
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 65 (4) , 1485-1500
- https://doi.org/10.1063/1.433202
Abstract
A program for calculating diatomic molecule absorption coefficients using ’’exact’’ numerically computed radial wavefunctions was developed and used to examine critically a number of approximations which are frequently used in absorption coefficient calculations. These tests showed that both use of the delta function approximation, and fixing the rotational quantum number in the radial overlap integrals at J=0, introduce errors of ?4%–6% of the absorption coefficient maximum εmax. Similarly, errors of ?1%–2% of εmax are introduced by either fixing the initial state J at the average value for the given temperature, or by using Gislason’s Airy‐function approximation for the unbound state wavefunction. A simple procedure for shrinking the sum over initial state J’s without significant loss of accuracy was therefore devised. These techniques were then applied to the analysis of the visible absorption continuum of Br2, and a nonlinear least‐squares fitting procedure used to determine optimized final state potential curves and transition moment functions for the two overlapping electronic transitions. In the region to which the data are sensitive, 2.10≲R≲2.55 Å, the transition moments so obtained (in debyes, lengths in angstroms) are M0(R) =0.3905+0.265(R−2.3) for the B (3Π+Ou) ←X (1Σ+g) transitions and M1(R) =0.5060–0.154(R−2.3) for the 1Π1u←X (1Σ+g) spectrum. The concomitant repulsive potential curves for the B (3Π+Ou) and 1Π1u states are, respectively (in cm−1, expressed relative to the ground state dissociation limit; lengths in angstroms): V0(R) =−1174+5494 exp[−5.807(R−2.3)] and V1(R) =7654 exp[−4.637(R−2.3)−0.879(R−2.3)2], where the former expression applies only to the region inside the B‐state inner turning point for v=8, R1(8) =2.4485 Å. Comparisons with experimental relative intensities in the discrete portion of the B–X spectrum, and with molecular beam photofragment spectroscopy measurements of the relative strengths of the two electronic transitions, are also reported.Keywords
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