Abstract
In working out nuclear energy levels on the Hartree approximation one meets certain integrals involving the interaction potential and the particle radial wave-functions (see parts I and II by H. A. Jahn (1950, 1951) in the present series). In this note these integrals are defined and worked out for the 1s, 2p, 3d wave-functions of a three-dimensional oscillator using as interaction potential (a) the Gauss potential, (b) the meson potential.

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