Application of a Higher RPA to a Model π‐Electron System
1.D. J. Rowe, Rev. Mod. Phys. 40, 153 (1968).
2.T. H. Dunning and V. McKoy, J. Chem. Phys. 47, 1735 (1967);
2.T. H. Dunning and V. McKoy, 48, 5263 (1968)., J. Chem. Phys.
3.T. Shibuya and V. McKoy, “Higher Random‐Phase Approximation as an Approximation to the Equations of Motion,” Phys. Rev. (to be published).
4.M. A. Ball and A. D. McLachlan, Mol. Phys. 7, 501 (1964).
5.We have used the Hartree atomic units throughout the paper unless otherwise indicated.
6.T. Shibuya and V. McKoy, “Application of the RPA and Higher RPA to the V and T states of Ethylene,” J. Chem. Phys. (to be published).
7.A set of three s‐like and two p‐like Gaussian orbitals on the carbon atom obtained by contraction from a set of nine s‐like and five p‐like GTO. The hydrogen basis is a single contracted orbital derived from four s‐like functions. See N. W. Winter, T. H. Dunning, Jr., and V. McKoy, J. Chem. Phys. 49, 4128 (1968).
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