Proceedings of the First International Symposium on Cyclodextrins 1982
DOI: 10.1007/978-94-009-7855-3_22
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A Simple Rule for Predicting Circular Dichroism Induced in Aromatic Guests by Cyclodextrin Hosts in Inclusion Complexes

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Cited by 79 publications
(100 citation statements)
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“…As can be seen from Figure 3, the circular dichroism spectrum of 1 showed a strong positive Cotton effect, which corresponds to the 1 L a band at 241 nm (De = 0.70 dm À3 mol À1 cm À1 ) and a negative Cotton effect for the 1 L b band at 269 nm (De = À0.23 dm À3 mol À1 cm À1 ). According to the pioneering studies of Kajtµr et al [21] and Harata and Uedaira [22] on the ICD phenomena of cyclodextrin complexes, we can deduce that the DPD moiety of 1 has entered into the b-CD cavity with a slightly acclivitous orientation, which is consistent with that seen in the crystal structure of 1. Interestingly, the DPD molecule in the b-CD cavity tethered by a Ni II ion gives an opposite ICD signal: a major negative Cotton effect at 232 nm (De = …”
supporting
confidence: 71%
“…As can be seen from Figure 3, the circular dichroism spectrum of 1 showed a strong positive Cotton effect, which corresponds to the 1 L a band at 241 nm (De = 0.70 dm À3 mol À1 cm À1 ) and a negative Cotton effect for the 1 L b band at 269 nm (De = À0.23 dm À3 mol À1 cm À1 ). According to the pioneering studies of Kajtµr et al [21] and Harata and Uedaira [22] on the ICD phenomena of cyclodextrin complexes, we can deduce that the DPD moiety of 1 has entered into the b-CD cavity with a slightly acclivitous orientation, which is consistent with that seen in the crystal structure of 1. Interestingly, the DPD molecule in the b-CD cavity tethered by a Ni II ion gives an opposite ICD signal: a major negative Cotton effect at 232 nm (De = …”
supporting
confidence: 71%
“…[23] From a comparison of the weak ICD spectra obtained for bis(b-cyclodextrin)s 2 ± 5 with that of the reference 6, we deduce that the bipyridine chromophore in 4 and 5 is not embedded in the cavity, while the chromophore in 2 and 3 is either perched on the edge of the cavity or shallowly penetrating into the cavity. Hence, the 1 L a transition of 2 and 3 is deduced to be located in the negative region of the sector rule proposed by Kajtar, [24] Harata, [25] and Kodaka et al, [26] while the weak, positive Cotton effect observed for the 1 L b band of 4 and 5 would be better analyzed as an ordinary CD induced by the two distant chiral cyclodextrin moieties, although a shallow binding or perching model is not rigorously ruled out.…”
Section: Resultsmentioning
confidence: 99%
“…According to the rule, a positive ICD signal arises when the electric transition dipole moment is aligned parallel to the axis of the chiral host, but the signal is negative and half as strong when it is oriented in a perpendicular manner ( Figure 5). [18][19][20][21] Recently, a similar rule has also been developed by Kodaka for ICD effects outside the chiral host cavity, where the sign of the ICD signal is opposite to that arising inside the host cavity ( Figure 5). [22] The prolonged irradiation of aqueous R1-alk solution (10 mol solid Na 2 CO 3 were added to the R1 and the isophthalic acid unit was changed to the anionic form) at 335 nm would result in the photoisomerization of the E to Z form and the shuttling of the a-CyD ring from the stilbene unit to the biphenyl unit, which was previously confirmed by 2D ROESY NMR spectrum.…”
Section: Synthesis and Co-conformational Identification Of R4mentioning
confidence: 99%