The first two lithium silenides, Li(tBu(2)MeSi)Si═C(SiMetBu(2))(1-Ad) (1) and Li(tBuMe(2)Si)Si═C(SiMetBu(2))(1-Ad) (2) were prepared by THF addition to the corresponding lithium-silenolates, [(tBu(2)MeSi)(2)Si═C(OLi)(1-Ad)]·(R(3)SiLi) (3a: R(3)Si═tBu(2)MeSi, 3b: R(3)Si═tBuMe(2)Si). 1 and 2 were crystallized, and their structures were determined by X-ray crystallography. This process requires the presence of both coaggregated silyllithium (R(3)SiLi) (3a and 3b) and THF. Based on reaction products and DFT calculations, it is suggested that elimination of tBu(2)MeSiOLi from 3a (or 3b) produces first the corresponding silyne intermediate which rearranges to the corresponding silylidene, which is then trapped by R(3)SiLi giving 1 (or 2).

Peptoids, N-substituted glycine oligomers, are an important class of foldamers that can adopt polyproline-type helices (PP-I and PP-II), given that the majority of their sequence consists of chiral, bulky side chains. Herein a new approach for the stabilization of a pure PP-I-like peptoid helix through metal coordination is introduced. A systematic spectroscopic study was performed on a series of peptoid heptamers bearing two 8-hydroxyquinoline ligands at fixed positions, and a mixture of chiral benzyl and alkyl substituents in varied positions along the peptoid backbone. When the benzyl groups are located at the 3rd and 4th positions, the peptoid (7P6) gives upon Cu binding a circular dichroism (CD) signal similar to that of a PP-I helix. Exciton couplet CD spectroscopy and EPR spectroscopy, as well as modifications to the length of 7P6 and derivatization through acetylation provided insights into the unique folding of 7P6 upon Cu binding, showing that it is led by two competing driving forces, namely coordination geometry and sequence.

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The understanding of structure–function relationships within synthetic biomimetic systems is a fundamental challenge in chemistry. Herein we report the direct correlation between the structure of short peptoid ligands—N‐substituted glycine oligomers incorporating 2,2′‐bipyridine groups—varied in their monomer sequence, and the photoluminescence of RuII centers coordinated by these ligands. Based on circular dichroism and fluorescence spectroscopy we demonstrate that while helical peptoids do not affect the fluorescence of the embedded RuII chromophore, unstructured peptoids lead to its significant decay. Transmittance electron microscopy (TEM) revealed significant differences in the arrangements of metal‐bound helical versus unstructured peptoids, suggesting that only the latter can have through‐space interactions with the ruthenium dye leading to its quenching. High‐resolution TEM enabled the remarkable direct imaging of singular ruthenium‐bound peptoids and bundles, supporting our explanation for structure‐depended quenching. Moreover, this correlation allowed us to fine‐tune the luminescence properties of the complexes simply by modifying the sequence of their peptoid ligands. Finally, we also describe the chiral properties of these Ru–peptoids and demonstrate that remote chiral induction from the peptoids backbone to the ruthenium center is only possible when the peptoids are both chiral and helical.

The worrysome development and spread of multidrug-resistant bacteria demands new antibacterial agents with strong bioactivities particularly against Gram−negative bacteria. Albicidins were recently structurally characterized as highly active antibacterial natural products...