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Higher order roots kna and q na (n, 2, 3, 4, ) correspond to higher-energy nS states. Corresponding wavefunctions have the same form as those in eq 1. Our calculations can be extended to these nS states by simply replacing the IS wavefunction with the nS wavefunctions
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a (n = 2, 3, 4, ...) correspond to higher-energy nS states. Corresponding wavefunctions have the same form as those in eq 1. Our calculations can be extended to these nS states by simply replacing the IS wavefunction with the nS wavefunctions.
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