Department of Chemistry, University of Waterloo , Waterloo, Ontario N2L 3G1, Canada.
J Am Chem Soc. 2014 Jun 4;136(22):8050-62. doi: 10.1021/ja502753t. Epub 2014 May 22.
The heterocyclic bisdithiazolyl radical 1b (R1 = Me, R2 = F) crystallizes in two phases. The α-phase, space group P2₁/n, contains two radicals in the asymmetric unit, both of which adopt slipped π-stack structures. The β-phase, space group P2₁/c, consists of cross-braced π-stacked arrays of dimers in which the radicals are linked laterally by hypervalent 4-center 6-electron S···S-S···S σ-bonds. Variable-temperature magnetic susceptibility measurements on α-1b indicate Curie-Weiss behavior (with Θ = -14.9 K), while the dimer phase β-1b is diamagnetic, showing no indication of thermal dissociation below 400 K. High-pressure crystallographic measurements indicate that the cross-braced π-stacked arrays of dimers undergo a wine-rack compression, but the dimer remains intact up to 8 GPa (at ambient temperature). The resistance of β-1b to dissociate under pressure, also observed in its conductivity versus pressure profile, is in marked contrast to the behavior of the related dimer β-1a (R1 = Et, R2 = F), which readily dissociates into a pair of radicals at 0.8 GPa. The different response of the two dimers to pressure has been rationalized in terms of differences in their linear compressibilities occasioned by changes in the degree of cross-bracing of the π-stacks. Dissociation of both dimers can be effected by irradiation with visible (λ = 650 nm) light; the transformation has been monitored by optical spectroscopy, magnetic susceptibility measurements, and single crystal X-ray diffraction. The photoinduced radical pairs persist up to temperatures of 150 K (β-1b) and 242 K (β-1a) before reverting to the dimer state. Variable-temperature optical measurements on β-1b and β-1a have afforded Arrhenius activation energies of 8.3 and 19.6 kcal mol(-1), respectively, for the radical-to-dimer reconversion. DFT and CAS-SCF calculations have been used to probe the ground and excited electronic state structures of the dimer and radical pair. The results support the interpretation that the ground-state interconversion of the dimer and radical forms of β-1a and β-1b is symmetry forbidden, while the photochemical transformation is symmetry allowed.
杂环双二硫杂环戊二烯基自由基 1b(R1 = Me,R2 = F)结晶为两相。α-相,空间群为 P2₁/n,在不对称单元中包含两个自由基,两者均采用错开的π-堆叠结构。β-相,空间群为 P2₁/c,由交叉支撑的二聚体π-堆叠阵列组成,其中自由基通过超价 4 中心 6 电子 S···S-S···S σ 键横向连接。对α-1b 的变温磁化率测量表明存在居里-外斯行为(Θ = -14.9 K),而二聚体相β-1b 为抗磁性,在 400 K 以下没有热离解的迹象。高压晶体学测量表明,交叉支撑的二聚体π-堆叠阵列发生酒架压缩,但二聚体在 8 GPa(环境温度下)以下仍保持完整。β-1b 在压力下不易离解,这在其电导率与压力关系图中也有体现,与相关二聚体β-1a(R1 = Et,R2 = F)的行为形成鲜明对比,后者在 0.8 GPa 下容易离解为一对自由基。两个二聚体对压力的不同反应可以用π-堆叠的交叉支撑程度变化引起的线性压缩率的差异来解释。可见光(λ = 650nm)照射即可使两个二聚体解离;通过光学光谱、磁化率测量和单晶 X 射线衍射监测了转变。光诱导自由基对在 150 K(β-1b)和 242 K(β-1a)之前的温度下保持稳定,然后再回到二聚体状态。对β-1b 和 β-1a 的变温光学测量分别给出了自由基-二聚体重新转化的 Arrhenius 活化能为 8.3 和 19.6 kcal mol(-1)。DFT 和 CAS-SCF 计算被用于研究二聚体和自由基对的基态和激发态电子结构。结果支持了这样的解释,即β-1a 和 β-1b 的二聚体和自由基形式的基态互变是对称性禁止的,而光化学转化是对称性允许的。