A general theoretical approach to the calculation of electronic excited states for molecules is described. A good ground state is not required and the method allows for arbitrary multiplicity of the states.
D. R. Armstrong, R. Fortune, P. G. Perkins and J. J. P. Stewart, J. Chem. Soc., Faraday Trans. 2, 1972, 68, 1839 DOI: 10.1039/F29726801839
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