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Chirality Induction in a Hydrophilic Metallohelicate
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AbstractThe title compound is a water‐soluble triply stranded metallohelicate 1Fe composed of TEG‐chain‐installed calix[4]arene‐based bis‐bidentate ligands and Fe3+ cations. This compound can incorporate up to two molecules of small chiral cations (G1 and G2). Interestingly, G1 shows positive cooperativity for host‐guest complexation, whereas G2 exhibits noncooperativity, despite having a greater affinity for 1Fe than G1. Density functional theory (DFT) calculations indicate the metallohelicate cavity expands upon encapsulation of the first guest. This conformational change facilitates the entrapment of the second guest and explains why the interaction parameters of G1 and G2 are larger than 1, despite electrostatic repulsion between the guests. The DFT calculation predicts an intermolecular interaction between the phenyl groups of G1 in the cavity, whereas no such interaction is found for G2. This difference can explain the distinct molecular recognition of G1 and G2. CD spectroscopy shows that both (R)‐G1 and (R)‐G2 induce (M)‐helicity in 1Fe and vice versa. DFT calculations suggest that the chirality of the guests is transmitted to 1Fe via CH/O hydrogen bonds between the guest and the C=O bond on the calix[4]arene strand. The CD intensity of 1Fe is nonlinear in the ee% of (R)‐ and (S)‐G1, indicating that the presence of the first guest increases the affinity of 1Fe toward a second guest with the same chirality due to preorganization by the first guest.
Title: Chirality Induction in a Hydrophilic Metallohelicate
Description:
AbstractThe title compound is a water‐soluble triply stranded metallohelicate 1Fe composed of TEG‐chain‐installed calix[4]arene‐based bis‐bidentate ligands and Fe3+ cations.
This compound can incorporate up to two molecules of small chiral cations (G1 and G2).
Interestingly, G1 shows positive cooperativity for host‐guest complexation, whereas G2 exhibits noncooperativity, despite having a greater affinity for 1Fe than G1.
Density functional theory (DFT) calculations indicate the metallohelicate cavity expands upon encapsulation of the first guest.
This conformational change facilitates the entrapment of the second guest and explains why the interaction parameters of G1 and G2 are larger than 1, despite electrostatic repulsion between the guests.
The DFT calculation predicts an intermolecular interaction between the phenyl groups of G1 in the cavity, whereas no such interaction is found for G2.
This difference can explain the distinct molecular recognition of G1 and G2.
CD spectroscopy shows that both (R)‐G1 and (R)‐G2 induce (M)‐helicity in 1Fe and vice versa.
DFT calculations suggest that the chirality of the guests is transmitted to 1Fe via CH/O hydrogen bonds between the guest and the C=O bond on the calix[4]arene strand.
The CD intensity of 1Fe is nonlinear in the ee% of (R)‐ and (S)‐G1, indicating that the presence of the first guest increases the affinity of 1Fe toward a second guest with the same chirality due to preorganization by the first guest.
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