Beer Leanne, Brusso Jaclyn L, Cordes A Wallace, Haddon Robert C, Itkis Mikhail E, Kirschbaum Kristin, MacGregor Douglas S, Oakley Richard T, Pinkerton A Alan, Reed Robert W
Contribution from the Department of Chemistry, University of Waterloo, Ontario N2L 3G1, Canada.
J Am Chem Soc. 2002 Aug 14;124(32):9498-509. doi: 10.1021/ja026118s.
Alkylation of the zwitterionic heterocycle 8-chloro-bis[1,2,3]dithiazolo[4,5-b:5',4'-e]pyridine (ClBP) with alkyl triflates affords 8-chloro-4-alkyl-4H-bis[1,2,3]dithiazolo[4,5-b:5',4'-e]pyridin-2-ium triflates [ClBPR][OTf] (R = Me, Et, Pr). Reduction of these salts with decamethylferrocene affords the corresponding ClBPR radicals as thermally stable crystalline solids. The radicals have been characterized in solution by cyclic voltammetry and EPR spectroscopy. Measured electrochemical cell potentials and computed (B3LYP/6-31G) gas-phase disproportionation enthalpies are consistent with a low on-site Coulombic barrier U to charge transfer in the solid state. The crystal structures of ClBPR (R = Me, Et, Pr) have been determined by X-ray crystallography (at 293 K). All three structures consist of slipped pi-stacks of undimerized radicals, with many close intermolecular S.S contacts. ClBPMe undergoes a phase transition at 93 K to a slightly modified slipped pi-stack arrangement, the structure of which has also been established crystallographically (at 25 K). Variable-temperature magnetic and conductivity measurements have been performed, and the results interpreted in light of extended Hückel band calculations. The room-temperature conductivities of ClBPR systems (sigma(RT) approximately 10(-)(5) to 10(-)(6) S cm(-)(1)), as well as the weak 1D ferromagnetism exhibited by ClBPMe, are interpreted in terms of weak intermolecular overlap along the pi-stacks. The latter is caused by slippage of the molecular plates, a feature necessitated by the steric size of the R and Cl groups on the pyridine ring.
两性离子杂环8-氯-双[1,2,3]二噻唑并[4,5-b:5',4'-e]吡啶(ClBP)与烷基三氟甲磺酸酯发生烷基化反应,生成8-氯-4-烷基-4H-双[1,2,3]二噻唑并[4,5-b:5',4'-e]吡啶-2-鎓三氟甲磺酸盐[ClBPR][OTf](R = 甲基、乙基、丙基)。用十甲基二茂铁还原这些盐,得到相应的ClBPR自由基,为热稳定的结晶固体。这些自由基已通过循环伏安法和电子顺磁共振光谱在溶液中进行了表征。测量的电化学电池电位和计算(B3LYP/6-31G)的气相歧化焓与固态中电荷转移的低原位库仑势垒U一致。已通过X射线晶体学(在293 K)确定了ClBPR(R = 甲基、乙基、丙基)的晶体结构。所有三种结构均由未二聚化自由基的滑移π堆积组成,具有许多紧密的分子间S···S接触。ClBPMe在93 K发生相变,转变为略有改变的滑移π堆积排列,其结构也已通过晶体学确定(在25 K)。已进行了变温磁性和电导率测量,并根据扩展休克尔能带计算对结果进行了解释。ClBPR体系的室温电导率(σ(RT)约为10⁻⁵至10⁻⁶ S cm⁻¹)以及ClBPMe表现出的弱一维铁磁性,是根据沿π堆积的弱分子间重叠来解释的。后者是由分子片的滑移引起的,这是吡啶环上R和Cl基团的空间尺寸所必需的特征。