Abstract
Using the “molecular puff” equations as a starting point, first‐order perturbation equations are solved for H2, HeH+, He22, and linear symmetric H3+, and first‐ and second‐order equations for H2+ and HeH2+. The perturbation wavefunctions are expanded in partial waves and the resulting equations solved by numerical integration for the 1sσ ground states. The errors in the calculated energies are in the range 0.5–10.0 kcal/mol and represent a considerable improvement on similar calculations reported by Hauck, Kim, Parr, and Hameka [J. Chem. Phys. 47, 2677 (1967)].

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