8-fluoro-4-pentyl-4H-bis([1,2,3]dithiazolo)[4,5-b:5′,4′-e]pyridin-2-ium trifluoromethanesulfonate | 1422660-28-3

• 分子结构分类: 有机化合物 - 有机卤素化合物 - 芳基卤化物
• 英文名称: 8-fluoro-4-pentyl-4H-bis([1,2,3]dithiazolo)[4,5-b:5′,4′-e]pyridin-2-ium trifluoromethanesulfonate
• CAS: 1422660-28-3
• 化学式: CF₃O₃S*C₁₀H₁₁FN₃S₄
• 分子量: 469.55
• InChiKey: KDZOVEHMEZQQEV-UHFFFAOYSA-M

计算性质

• 辛醇/水分配系数(LogP)：
  4.89
• 重原子数：
  26.0
• 可旋转键数：
  4.0
• 环数：
  3.0
• sp3杂化的碳原子比例：
  0.55
• 拓扑面积：
  85.69
• 氢给体数：
  0.0
• 氢受体数：
  9.0

反应信息

• 作为反应物：
  描述：

  8-fluoro-4-pentyl-4H-bis([1,2,3]dithiazolo)[4,5-b:5′,4′-e]pyridin-2-ium trifluoromethanesulfonate 在 bis(pentamethylcyclopentadienyl)iron(II) 作用下， 以 乙腈 为溶剂， 反应 2.0h， 以79%的产率得到8-fluoro-4-pentyl-4H-bis([1,2,3]dithiazolo)[4,5-b:5′,4′-e]pyridin-2-yl
  参考文献：
  名称：

  Bisdithiazolyl Radical Spin Ladders

  摘要：

  A series of four bisdithiazolyl radicals 1a-d (R-1 = Pr, Bu, Pn, Hx; R-2 = F) has been prepared and characterized by X-ray crystallography. The crystal structure of 1a (R-1 = Pr) belongs to the tetragonal space group P (4) over bar2(1)m and consists of slipped pi-stack arrays of undimerized radicals packed about (4) over bar centers running along the z-direction, an arrangement identical to that found for 1 (R-1 = Et; R-2 = F). With increasing chain length of the R-1 substituent, an isomorphous set 1b-d is generated. All three compounds crystallize in the P2(1)/c space group and consist of pairs of radical pi-stacks locked together by strong intermolecular F center dot center dot center dot S' bridges to create spin ladder arrays. The slipped pi-stack alignment of radicals produces close S center dot center dot center dot S' interactions which serve as the "rungs" of a spin ladder, and the long chain alkyl substituents (R-1) serve as buffers which separate the ladders from each other laterally. Variable temperature magnetic susceptibility measurements indicate that la behaves as an antiferromagnetically coupled Curie-Weiss paramagnet, the behavior of which may be modeled as a weakly coupled AFM chain. Stronger antiferromagnetic coupling is observed in 1b-d, such that the Curie-Weiss fit is no longer applicable. Analysis of the full data range (T = 2-300 K) is consistent with the Johnston strong-leg spin ladder model. The origin of the magnetic behavior across the series has been explored with broken-symmetry Density Functional Theory (DFT) calculations of individual pairwise exchange energies. These confirm that strong antiferromagnetic interactions are present within the ladder "legs" and "rungs", with only very weak magnetic exchange between the ladders.

  DOI：

  10.1021/ic302658c
• 作为产物：
  描述：

  N-pentyl-2,6-diamino-4-fluoropyridinium trifluoromethanesulfonate 在 二氯化二硫 作用下， 以 1,2-二氯乙烷 、 乙腈 为溶剂， 反应 2.5h， 以46%的产率得到8-fluoro-4-pentyl-4H-bis([1,2,3]dithiazolo)[4,5-b:5′,4′-e]pyridin-2-ium trifluoromethanesulfonate
  参考文献：
  名称：

  Bisdithiazolyl Radical Spin Ladders

  摘要：

  A series of four bisdithiazolyl radicals 1a-d (R-1 = Pr, Bu, Pn, Hx; R-2 = F) has been prepared and characterized by X-ray crystallography. The crystal structure of 1a (R-1 = Pr) belongs to the tetragonal space group P (4) over bar2(1)m and consists of slipped pi-stack arrays of undimerized radicals packed about (4) over bar centers running along the z-direction, an arrangement identical to that found for 1 (R-1 = Et; R-2 = F). With increasing chain length of the R-1 substituent, an isomorphous set 1b-d is generated. All three compounds crystallize in the P2(1)/c space group and consist of pairs of radical pi-stacks locked together by strong intermolecular F center dot center dot center dot S' bridges to create spin ladder arrays. The slipped pi-stack alignment of radicals produces close S center dot center dot center dot S' interactions which serve as the "rungs" of a spin ladder, and the long chain alkyl substituents (R-1) serve as buffers which separate the ladders from each other laterally. Variable temperature magnetic susceptibility measurements indicate that la behaves as an antiferromagnetically coupled Curie-Weiss paramagnet, the behavior of which may be modeled as a weakly coupled AFM chain. Stronger antiferromagnetic coupling is observed in 1b-d, such that the Curie-Weiss fit is no longer applicable. Analysis of the full data range (T = 2-300 K) is consistent with the Johnston strong-leg spin ladder model. The origin of the magnetic behavior across the series has been explored with broken-symmetry Density Functional Theory (DFT) calculations of individual pairwise exchange energies. These confirm that strong antiferromagnetic interactions are present within the ladder "legs" and "rungs", with only very weak magnetic exchange between the ladders.

  DOI：

  10.1021/ic302658c