FBPMe | 1610336-13-4

• 分子结构分类: 有机化合物 - 苯类化合物 - 苯和取代衍生物
• 英文名称: FBPMe
• 英文别名: (5E)-7-fluoro-5-[[(E)-(7-fluoro-4-methyl-6-sulfanylidenedithiazolo[4,5-b]pyridin-5-ylidene)amino]disulfanyl]imino-4-methyldithiazolo[4,5-b]pyridine-6-thione
• CAS: 1610336-13-4
• 化学式: C₁₂H₆F₂N₆S₈
• 分子量: 528.745
• InChiKey: MYBVMOQGNSWPGS-KAVGSWPWSA-N

计算性质

• 辛醇/水分配系数(LogP)：
  3.6
• 重原子数：
  28
• 可旋转键数：
  3
• 环数：
  4.0
• sp3杂化的碳原子比例：
  0.17
• 拓扑面积：
  272
• 氢给体数：
  0
• 氢受体数：
  14

反应信息

• 作为反应物：
  描述：

  FBPMe 106.84 ℃ 、800.01 MPa 条件下， 生成 8-fluoro-4-methyl-4H-bis[1,2,3]dithiazolo[4,5-b:5,4-e]pyridin-3-yl
  参考文献：
  名称：

  Heat, Pressure and Light-Induced Interconversion of Bisdithiazolyl Radicals and Dimers

  摘要：

  The heterocyclic bisdithiazolyl radical 1b (R-1 = Me, R-2 = F) crystallizes in two phases. The alpha-phase, space group P2(1)/n, contains two radicals in the asymmetric unit, both of which adopt slipped pi-stack structures. The beta-phase, space group P2(1)/c, consists of cross-braced pi-stacked arrays of dimers in which the radicals are linked laterally by hypervalent 4-center 6-electron S center dot center dot center dot S-S center dot center dot center dot S sigma-bonds. Variable-temperature magnetic susceptibility measurements on alpha-1b indicate Curie-Weiss behavior (with Theta = -14.9 K), while the dimer phase beta-1b is diamagnetic, showing no indication of thermal dissociation below 400 K. High-pressure crystallographic measurements indicate that the cross-braced pi-stacked arrays of dimers undergo a wine-rack compression, but the dimer remains intact up to 8 GPa (at ambient temperature). The resistance of beta-1b to dissociate under pressure, also observed in its conductivity versus pressure profile, is in marked contrast to the behavior of the related dimer beta-1a (R-1 = Et, R-2 = 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 pi-stacks. Dissociation of both dimers can be effected by irradiation with visible (lambda = 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 (beta-1b) and 242 K (beta-1a) before reverting to the dimer state. Variable-temperature optical measurements on beta-1b and beta-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 beta-1a and beta-1b is symmetry forbidden, while the photochemical transformation is symmetry allowed.

  DOI：

  10.1021/ja502753t
• 作为产物：
  描述：

  在 bis(pentamethylcyclopentadienyl)iron(II) 作用下， 以 乙腈 为溶剂， 反应 4.0h， 以84%的产率得到8-fluoro-4-methyl-4H-bis[1,2,3]dithiazolo[4,5-b:5,4-e]pyridin-3-yl
  参考文献：
  名称：

  Heat, Pressure and Light-Induced Interconversion of Bisdithiazolyl Radicals and Dimers

  摘要：

  The heterocyclic bisdithiazolyl radical 1b (R-1 = Me, R-2 = F) crystallizes in two phases. The alpha-phase, space group P2(1)/n, contains two radicals in the asymmetric unit, both of which adopt slipped pi-stack structures. The beta-phase, space group P2(1)/c, consists of cross-braced pi-stacked arrays of dimers in which the radicals are linked laterally by hypervalent 4-center 6-electron S center dot center dot center dot S-S center dot center dot center dot S sigma-bonds. Variable-temperature magnetic susceptibility measurements on alpha-1b indicate Curie-Weiss behavior (with Theta = -14.9 K), while the dimer phase beta-1b is diamagnetic, showing no indication of thermal dissociation below 400 K. High-pressure crystallographic measurements indicate that the cross-braced pi-stacked arrays of dimers undergo a wine-rack compression, but the dimer remains intact up to 8 GPa (at ambient temperature). The resistance of beta-1b to dissociate under pressure, also observed in its conductivity versus pressure profile, is in marked contrast to the behavior of the related dimer beta-1a (R-1 = Et, R-2 = 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 pi-stacks. Dissociation of both dimers can be effected by irradiation with visible (lambda = 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 (beta-1b) and 242 K (beta-1a) before reverting to the dimer state. Variable-temperature optical measurements on beta-1b and beta-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 beta-1a and beta-1b is symmetry forbidden, while the photochemical transformation is symmetry allowed.

  DOI：

  10.1021/ja502753t