Absolute helical arrangement of stacked benzene rings: heterogeneous double-helical interaction comprising a hydrogen-bonding belt and an offset parallel aromatic-aromatic-interaction array.
Absolute helical arrangement of stacked benzene rings: heterogeneous double-helical interaction comprising a hydrogen-bonding belt and an offset parallel aromatic-aromatic-interaction array.
复制标题
DOI:
10.1002/anie.200352788
复制
发表时间:
2004-03
影响因子:
--
通讯作者:
I. Azumaya;D. Uchida;Takako Kato;A. Yokoyama;Aya Tanatani;H. Takayanagi;T. Yokozawa
中科院分区:
文献类型:
--
作者:
I. Azumaya;D. Uchida;Takako Kato;A. Yokoyama;Aya Tanatani;H. Takayanagi;T. Yokozawa
Compounds that form helical structures in the crystalline state or in solution [1] have attracted much attention because living things utilize helical structures to store genetic information, and because compounds with a helical-ordered structure have provided new materials in solid-or liquidcrystal engineering.[2] There are several types of helical structure: a single strand that folds helically owing to solvophobic effect [3] or guest ligation,[4] a double or multiple helix of strands derived from cation or anion ligation,[5] or hydrogen bonding,[6] and a helical super-structure formed by conformationally helical or discotic small molecules through columnar stacking supported by hydrogen bonds,[7] for other examples see ref.[8]. In helical structures, a parallel aromatic–aromatic interaction [9] is often a very important driving force to stabilize the structure, and sometimes hydrogen bonding or other weak intermolecular interactions assist the formation of the highly ordered helical arrangement. Such a helical structure is intrinsically chiral, that is, it has a righthanded helix (P-helix) or a left-handed helix (M-helix), which are enantiomeric. Asymmetric synthesis to produce one enantiomeric helix is important, especially in self-assembling systems,[5–7] in foldamers,[1a] or in polymers with a helical structure induced by catalytic chiral initiation.[10] There are generally two kinds of driving forces to determine which helicity a compound will adopt, they are, an internal or an external chiral source. For example, the helicity of DNA is derived from the internal chirality of the chiral carbon atom in the deoxyribose chain. On the other hand, one of oligophenylacetylenes prepared by Moore and co-workers folded into a single helical form upon ligation of a chiral ligand.[4b, c] In this context, absolute asymmetric assembly of an achiral molecule is especially intriguing. In the course of our investigation [11] of spontaneous optical resolution,[12] we found a discotic compound, tris (2-hydroxyethyl)-1, 3, 5-benzenetricarboxylate (1), which crystallized as chiral crystals in which the nearly planar molecules were helically arranged within individual single crystals. The helicity of the triester 1 was derived from the helical arrangement of the molecules, supported by an array of hydrogen bonding through a single moiety and offset aromatic stacking of the adjacent molecules. The triester 1, which has an almost planar and highly symmetrical primary structure, was synthesized and crystallized from methanol/chloroform to give slender prismatic single crystals. A preliminary X-ray crystallographic analysis (Figure1) revealed that the crystal belonged to the noncentrosymmetric space group P61 (or P65). This result was surprising, since the majority of achiral organic compounds tend to pack into centrosymmetric crystals. The most interesting feature is that the planar, discotic molecules were arranged in a columnar stack with a progressive helical twist between adjacent molecules to form helical superstructures in the crystal lattice. The chirality of the crystals was intrinsically derived from the helical arrangement of the molecules, assisted by the twist of the terminal hydroxy groups with respect to the plane of the central benzene ring, which leads to the generation of conformational chirality. We measured the solid-state CD spectrum (in KBr) of several crystals of 1.[13] The Cotton effect was characteristic of a helical structure of a chromophore.[14] As expected, we found two enantiomeric crystals which showed mirror-image curves in the region between 200–320 nm (Figure 2); one (red line in Figure 2) showed a negative Cotton effect at around 210 nm, a large positive one at 224 nm, a negative one at 248 nm, and …