Abstract
Single‐center wavefunctions are constructed for the lowest‐lying singlet and triplet Πu(1sσ2pπ) and Πg(1sσ3dπ) excited states of the hydrogen molecule using a basis set of integral Slater‐type orbitals centered at the molecular midpoint. It is found that the convergence is more rapid than for a corresponding single‐center calculation on the ground state. The error in the binding energy is about 0.065 eV for the Πu states and 0.033 eV for the Πg states if a 19‐term configuration‐interaction wavefunction is used for the description of each.

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