The wavefunction of a low-energy unbound electron in the field of a closed-shell diatomic molecular ion is calculated using a single-centre expansion in the static-exchange approximation. The evaluation is reported of the electronic capture width necessary for the calculation of the dissociative-recombination rate of the CH + ion in its ground state, with a two-centre molecular integral program. The agreement between calculated values for a very low energy (0.01 eV) and extrapolated values from Rydberg states, found both for the quantum defect and the electronic-capture width, establishes the reliability of the direct calculation.
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Raşeev et al. (1978) studied this question.
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