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| 1354649-23-2

中文名称
——
中文别名
——
英文名称
——
英文别名
——
化学式
CAS
1354649-23-2
化学式
C6ClN2OS4
mdl
——
分子量
279.796
InChiKey
AHNSRDAYKKJXAD-UHFFFAOYSA-N
BEILSTEIN
——
EINECS
——
  • 物化性质
  • 计算性质
  • ADMET
  • 安全信息
  • SDS
  • 制备方法与用途
  • 上下游信息
  • 反应信息
  • 文献信息
  • 表征谱图
  • 同类化合物
  • 相关功能分类
  • 相关结构分类

计算性质

  • 辛醇/水分配系数(LogP):
    1.9
  • 重原子数:
    14
  • 可旋转键数:
    0
  • 环数:
    3.0
  • sp3杂化的碳原子比例:
    0.0
  • 拓扑面积:
    132
  • 氢给体数:
    0
  • 氢受体数:
    6

反应信息

  • 作为产物:
    描述:
    4-氯-2,6-二硝基苯酚盐酸二氯化二硫tin双(四甲基环戊二烯)铁 、 tin(II) chloride dihdyrate 作用下, 以 乙腈丙腈 为溶剂, 反应 4.0h, 生成
    参考文献:
    名称:
    Semiquinone-Bridged Bisdithiazolyl Radicals as Neutral Radical Conductors
    摘要:
    Semiquinone-bridged bisdithiazolyls 3 represent a new class of resonance-stabilized neutral radical for use in the design of single-component conductive materials. As such, they display electrochemical cell potentials lower than those of related pyridine-bridged bisdithiazolyls, a finding which heralds a reduced on-site Coulomb repulsion U. Crystallographic characterization of the chloro-substituted derivative 3a and its acetonitrile solvate 3a center dot MeCN, both of which crystallize in the polar orthorhombic space group Pna2(1), revealed the importance of intermolecular oxygen-to-sulfur (CO center dot center dot center dot SN) interactions in generating rigid, tightly packed radical pi-stacks, including the structural motif found for 3a center dot MeCN in which radicals in neighboring pi-stacks are locked into slipped-ribbon-like arrays. This architecture gives rise to strong intra- and interstack overlap and hence a large electronic bandwidth W. Variable-temperature conductivity measurements on 3a and 3a center dot MeCN indicated high values of sigma(300 K) (>10(-3) S cm(-1)) with correspondingly low thermal activation energies E-act, reaching 0.11 eV in the case of 3a center dot MeCN. Overall, the strong performance of these materials as f = 1/2 conductors is attributed to a combination of low U and large W. Variable-temperature magnetic susceptibility measurements were performed on both 3a and 3a center dot MeCN. The unsolvated material 3a orders as a spincanted antiferromagnet at 8 K, with a canting angle phi = 0.14 degrees and a coercive field H-c = 80 Oe at 2 K.
    DOI:
    10.1021/ja209841z
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文献信息

  • Semiquinone-Bridged Bisdithiazolyl Radicals as Neutral Radical Conductors
    作者:Xin Yu、Aaron Mailman、Kristina Lekin、Abdeljalil Assoud、Craig M. Robertson、Bruce C. Noll、Charles F. Campana、Judith A. K. Howard、Paul A. Dube、Richard T. Oakley
    DOI:10.1021/ja209841z
    日期:2012.2.1
    Semiquinone-bridged bisdithiazolyls 3 represent a new class of resonance-stabilized neutral radical for use in the design of single-component conductive materials. As such, they display electrochemical cell potentials lower than those of related pyridine-bridged bisdithiazolyls, a finding which heralds a reduced on-site Coulomb repulsion U. Crystallographic characterization of the chloro-substituted derivative 3a and its acetonitrile solvate 3a center dot MeCN, both of which crystallize in the polar orthorhombic space group Pna2(1), revealed the importance of intermolecular oxygen-to-sulfur (CO center dot center dot center dot SN) interactions in generating rigid, tightly packed radical pi-stacks, including the structural motif found for 3a center dot MeCN in which radicals in neighboring pi-stacks are locked into slipped-ribbon-like arrays. This architecture gives rise to strong intra- and interstack overlap and hence a large electronic bandwidth W. Variable-temperature conductivity measurements on 3a and 3a center dot MeCN indicated high values of sigma(300 K) (>10(-3) S cm(-1)) with correspondingly low thermal activation energies E-act, reaching 0.11 eV in the case of 3a center dot MeCN. Overall, the strong performance of these materials as f = 1/2 conductors is attributed to a combination of low U and large W. Variable-temperature magnetic susceptibility measurements were performed on both 3a and 3a center dot MeCN. The unsolvated material 3a orders as a spincanted antiferromagnet at 8 K, with a canting angle phi = 0.14 degrees and a coercive field H-c = 80 Oe at 2 K.
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