1970
DOI: 10.1135/cccc19701939
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Optical rotatory power of complex compounds. Matrix elements of the operators ∇ and (r x ∇)

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Cited by 10 publications
(5 citation statements)
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“…Let p = (ζ 1 + ζ 2 ) R /2, q = (ζ 2 − ζ 1 ) R /2, A k = w k exp(− pw ) d w and B k = w k exp(− qw ) d w . Then, following procedures described by Mulliken et al, Král, and Harada and Nakanishi, we find Equations A2 and A3 were given previously by Král …”
mentioning
confidence: 99%
“…Let p = (ζ 1 + ζ 2 ) R /2, q = (ζ 2 − ζ 1 ) R /2, A k = w k exp(− pw ) d w and B k = w k exp(− qw ) d w . Then, following procedures described by Mulliken et al, Král, and Harada and Nakanishi, we find Equations A2 and A3 were given previously by Král …”
mentioning
confidence: 99%
“…In fact, the combination y∂(2p z )/∂z À z∂(2p z )/∂y has exactly the same spatial distribution as 2p y [1,2]. the overlap of the two wavefunctions falls off with the interatomic distance.…”
Section: þmentioning
confidence: 87%
“…(9.32b) indicates, ℜ ex is extremely sensitive to the geometry of the dimer. It will be zero if any two of the three vectors (μ ba(1) , μ ba (2) , and R 21 ) are parallel or if all three vectors lie in the same plane.…”
Section: Circular Dichroism Of Dimers and Higher Oligomersmentioning
confidence: 99%
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