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bis[1,2,3]selenathiazolo[4,5-b:5',4'-e]pyridin-2-ium-4-ide | 951697-67-9

中文名称
——
中文别名
——
英文名称
bis[1,2,3]selenathiazolo[4,5-b:5',4'-e]pyridin-2-ium-4-ide
英文别名
——
bis[1,2,3]selenathiazolo[4,5-b:5',4'-e]pyridin-2-ium-4-ide化学式
CAS
951697-67-9;918156-42-0
化学式
C5HN3S2Se2
mdl
——
分子量
325.135
InChiKey
GOIXBIXNORPZRT-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):
    1.52
  • 重原子数:
    12.0
  • 可旋转键数:
    0.0
  • 环数:
    3.0
  • sp3杂化的碳原子比例:
    0.0
  • 拓扑面积:
    39.35
  • 氢给体数:
    0.0
  • 氢受体数:
    3.0

反应信息

  • 作为反应物:
    描述:
    bis[1,2,3]selenathiazolo[4,5-b:5',4'-e]pyridin-2-ium-4-ide 在 selenium(IV) oxide 作用下, 以 溶剂黄1461,2-二氯乙烷 为溶剂, 反应 1.5h, 生成
    参考文献:
    名称:
    Spin-canting in heavy atom heterocyclic radicals
    摘要:
    一对同构双硒噻唑基和双二硒唑基自由基导体表现出弱(自旋倾斜)铁磁性,Tc 值分别为 18 K 和 27 K。
    DOI:
    10.1039/b708756j
  • 作为产物:
    描述:
    4H-bis[1,2,3]selenathiazolo[4,5-b:5',4'-e]pyridin-2-ium trifluoromethanesulfonate 以 乙腈 为溶剂, 反应 16.0h, 以96%的产率得到bis[1,2,3]selenathiazolo[4,5-b:5',4'-e]pyridin-2-ium-4-ide
    参考文献:
    名称:
    Resonance Stabilized Bisdiselenazolyls as Neutral Radical Conductors
    摘要:
    An efficient and versatile synthetic route to resonance stabilized bisselenathiazolyl and bisdiselenazolyl radicals 3 and 4 is described. Structural analysis of 3 and 4 confirm that lattice and pi-delocalization energies are sufficient to offset solid-state dimerization of the radicals and that the two selenium-containing radicals are isostructural with the all-sulfur based system 1. Variable temperature conductivity measurements indicate that sequential replacement of sulfur by selenium leads to a progressive increase in conductivity and reduction in thermal activation energy.
    DOI:
    10.1021/ja0666856
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文献信息

  • Leiten, Allcea A.; Yu, Xueyang; Winter, Stephen M., Journal of the American Chemical Society, 2009, vol. 131, p. 7112 - 7125
    作者:Leiten, Allcea A.、Yu, Xueyang、Winter, Stephen M.、Secco, Richard A.、Dube, Paul A.、Oakley, Richard T.
    DOI:——
    日期:——
  • Enhanced Conductivity and Magnetic Ordering in Isostructural Heavy Atom Radicals
    作者:Craig M. Robertson、Alicea A. Leitch、Kristina Cvrkalj、Robert W. Reed、Daniel J. T. Myles、Paul A. Dube、Richard T. Oakley
    DOI:10.1021/ja801070d
    日期:2008.7.1
    Synthetic methods have been developed to generate the complete series of resonance-stabilized heterocyclic thia/selenazyl radicals 1a-4a. X-ray crystallographic studies confirm that all four radicals are isostructural, belonging to the tetragonal space group P (4) over bar2(1)m. The crystal structures consist of slipped pi-stack arrays of undimerized radicals packed about (4) over bar centers running along the z direction, an arrangement which gives rise to a complex lattice-wide network of close intermolecular E-2-E-2' contacts. Variable temperature conductivity (sigma) measurements reveal an increase in conductivity with increasing selenium content, particularly so When selenium occupies the E-2 position, with sigma(300 K) reaching a maximum (for E-1 = E-2 = Se) of 3.0 x 10(-4) S cm(-1). Thermal activation energies E-act follow a similar profile, decreasing with increasing selenium content along the series 1a (0.43 eV), 3a (0.31 eV), 2a (0.27 eV), 4a (0.19 eV). Variable temperature magnetic susceptibility measurements indicate that all four radicals exhibit S = 1/2 Curie-Weiss behavior over the temperature range 20-300 K. At lower temperatures, the three selenium-based radicals display magnetic ordering. Radical 3a, with selenium positioned at the E-1 site, undergoes a phase transition at 14 K to a weakly spin-canted (phi = 0.010 degrees) antiferromagnetic state. By contrast, radicals 2a and 4a, which both possess selenium in the E-2 position, order ferromagnetically, with Curie temperatures of T-c = 12.8 and 17.0 K, respectively. The coercive fields H-c at 2 K of 2a (250 Oe) and 4a (1370 Oe) are much larger than those seen in conventional light atom organic ferromagnets. The transport properties of the entire series 1a-4a are discussed in the light of Extended Huckel Theory band structure calculations.
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