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The Slater-type exponentialfunctions are, however, not adequate for the floating basis as they introduce unnecessary cusps in the free space between the nuclei
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The Slater-type exponentialfunctions are, however, not adequate for the floating basis as they introduce unnecessary cusps in the free space between the nuclei.
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Here we deal with a single VB configuration consisting of the perfect-pairing spin-couplings such as αβ-αβ and three others, and not with the resonance between the alternative spin-coupling configuration such as ααββ. Cases where the resonance is essential will be discussed elsewhere
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Here we deal with a single VB configuration consisting of the perfect-pairing spin-couplings such as αβ-αβ and three others, and not with the resonance between the alternative spin-coupling configuration such as ααββ. Cases where the resonance is essential will be discussed elsewhere.
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To quote from Ref. 54, ".a single Gaussian is such a poor representation of the cusp, (⋯), that an outer function will try to move on to the nucleus to improve the representation there rather than to routside and represent the more weakly bound electrons.
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