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Amplification of weak chiral inductions for excellent control over the helical orientation of discrete topologically chiral (M(3)L(2))(n) polyhedra
Superb control over the helical chirality of discrete (M(3)L(2))(n) polyhedra (n = 2,4,8, M = Cu(I) or Ag(I)) created from the self-assembly of propeller-shaped ligands (L) equipped with chiral side chains is demonstrated here. Almost perfect chiral induction (>99 : 1) of the helical orientation...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9006968/ https://www.ncbi.nlm.nih.gov/pubmed/35509455 http://dx.doi.org/10.1039/d2sc00111j |
Sumario: | Superb control over the helical chirality of discrete (M(3)L(2))(n) polyhedra (n = 2,4,8, M = Cu(I) or Ag(I)) created from the self-assembly of propeller-shaped ligands (L) equipped with chiral side chains is demonstrated here. Almost perfect chiral induction (>99 : 1) of the helical orientation of the framework was achieved for the largest (M(3)L(2))(8) cube with 48 small chiral side chains (diameter: ∼5 nm), while no or moderate chiral induction was observed for smaller polyhedra (n = 2, 4). Thus, amplification of the weak chiral inductions of each ligand unit is an efficient way to control the chirality of large discrete nanostructures with high structural complexity. |
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