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NBN 和 BNB-菲烯基:杂原子掺杂π体系的阴阳两面

NBN- and BNB-Phenalenyls: the Yin and Yang of Heteroatom-doped π Systems.

作者信息

Scholz Alexander S, Massoth Julian G, Stoess Lennart, Bolte Michael, Braun Markus, Lerner Hans-Wolfram, Mewes Jan-M, Wagner Matthias, Froitzheim Thomas

机构信息

Institut für Anorganische und Analytische Chemie, Goethe-Universität Frankfurt am Main, Max-von-Laue-Straße 7, 60438, Frankfurt am Main, Germany.

Institut für Physikalische und Theoretische Chemie, Goethe-Universität Frankfurt am Main, Max-von-Laue-Straße 7, 60438, Frankfurt am Main, Germany.

出版信息

Chemistry. 2024 May 14;30(27):e202400320. doi: 10.1002/chem.202400320. Epub 2024 Mar 19.

Abstract

NBN- and BNB-doped phenalenyls are isoelectronic to phenalenyl anions and cations, respectively. They represent a pair of complementary molecules that have essentially identical structures but opposite properties as electron donors and acceptors. The NBN-phenalenyls 1-4 considered here were prepared from N,N'-dimethyl-1,8-diaminonaphthalene and readily available boron-containing building blocks (i. e., BH⋅SMe (1), p-CF-CHB(OH) (2), CHB(OH) (3), or MesBCl/iPrNEt (4)). Treatment of 1 with 4-MeN-2,6-Me-CHLi gave the corresponding NBN derivative 5. The BNB-phenalenyl 6 was synthesized from 1,8-naphthalenediyl-bridged diborane(6), PhNH, and MesMgBr. A computational study reveals that the photoemission of 1, 4, and 5 originates from locally excited (LE) states at the NBN-phenalenyl fragments, while that of 2 is dominated by charge transfer (CT) from the NBN-phenalenyl to the p-CF-CH fragment. Depending on the dihedral angle θ between its Ph and NBN planes, compound 3 emits mainly from a less polar LE (θ >55°) or more polar CT state (θ <55°). In turn, the energetic preference for either state is governed by the polarity of the solvent used. An equimolar aggregate of the NBN- and BNB-phenalenyls 3 and 6 (in THF/HO) shows a distinct red-shifted emission compared to that of the individual components, which originates from an intermolecular CT state.

摘要

掺氮硼萘并萘与掺硼氮萘并萘分别与萘并萘阴离子和阳离子等电子。它们代表了一对互补分子,其结构基本相同,但作为电子供体和受体的性质相反。本文所考虑的掺氮硼萘并萘1 - 4由N,N'-二甲基-1,8 -二氨基萘和易于获得的含硼结构单元(即BH⋅SMe (1)、对三氟甲基苯硼酸 (2)、苯硼酸 (3) 或均三甲苯基氯化硼/二异丙基乙胺 (4))制备。用4 - 甲基氮杂-2,6 -二甲基苯锂处理1得到相应的掺氮硼衍生物5。掺硼氮萘并萘6由1,8 -萘二基桥连的乙硼烷(6)、苯胺和均三甲苯基溴化镁合成。一项计算研究表明,1、4和5的光发射源于掺氮硼萘并萘片段的局域激发(LE)态,而2的光发射主要由从掺氮硼萘并萘到对三氟甲基苯片段的电荷转移(CT)主导。根据其苯环和掺氮硼平面之间的二面角θ,化合物3主要从极性较小的LE态(θ >55°)或极性较大的CT态(θ <55°)发射。反过来,对任一态的能量偏好由所用溶剂的极性决定。掺氮硼萘并萘3和掺硼氮萘并萘6(在四氢呋喃/水中)的等摩尔聚集体与单个组分相比显示出明显的红移发射,这源于分子间CT态。

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