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1,9-Di-(2-thienyl)nonane | 38260-89-8

中文名称
——
中文别名
——
英文名称
1,9-Di-(2-thienyl)nonane
英文别名
——
1,9-Di-(2-thienyl)nonane化学式
CAS
38260-89-8
化学式
C17H24S2
mdl
——
分子量
292.51
InChiKey
XPWLCUMJIGKZJR-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

物化性质

  • 沸点:
    390.1±17.0 °C(Predicted)
  • 密度:
    1.054±0.06 g/cm3(Predicted)

计算性质

  • 辛醇/水分配系数(LogP):
    6.33
  • 重原子数:
    19.0
  • 可旋转键数:
    10.0
  • 环数:
    2.0
  • sp3杂化的碳原子比例:
    0.53
  • 拓扑面积:
    0.0
  • 氢给体数:
    0.0
  • 氢受体数:
    2.0

反应信息

  • 作为反应物:
    描述:
    1,9-Di-(2-thienyl)nonane正丁基锂potassium tert-butylate 作用下, 反应 16.0h, 生成 E,E-1,9-Bis<5-(2-fluorenylvinyl)-2-thienyl>nonane
    参考文献:
    名称:
    Kossmehl, Gerhard; Hoppe, Frank Dirk; Hirsch, Barbara, Zeitschrift fur Naturforschung, B: Chemical Sciences, 1993, vol. 48, # 6, p. 826 - 843
    摘要:
    DOI:
  • 作为产物:
    描述:
    噻吩1,10-二溴癸烷正丁基锂 作用下, 以 四氢呋喃 为溶剂, 生成 1,9-Di-(2-thienyl)nonane
    参考文献:
    名称:
    Complementary Semiconducting Polymer Blends: The Influence of Conjugation-Break Spacer Length in Matrix Polymers
    摘要:
    The concept of complementary semiconducting polymer blends (c-SPBs) for efficient charge transport was recently proposed and established by our group. In this study, we aim to reveal the influence of the length of conjugation-break spacers (CBSs) on charge transport properties of the matrix polymers and their corresponding complementary polymer blends. A series of 11 DPP-based semiconducting polymers DPP-Cm (m = 2-12) that incorporate CBSs of 2-12 methylene units along the polymer backbones were prepared and characterized. The UV vis spectra and the ultraviolet photoelectron spectroscopy (UPS) measurements show that the CBS length has marginal influence on the polymer absorption spectra, energy levels, and band gaps. It also has little impact on polymer decomposition temperatures. However, the CBS length has a profound influence on polymer phase transition and the heat of fusion. As for the melt transitions, an odd even effect is observed from DPP-C2 to DPP-C7, in which polymers with even-numbered CBSs show higher melting points than their adjacent odd-numbered derivatives. The trend is opposite for heat of fusion. The polymers with odd-numbered CBSs exhibit larger heat of fusion, indicating higher ordering and crystallinity. The odd even effect is also found in surface morphologies of the polymers by atomic force microscopy (AFM). The polymers with the even CBSs have a more interconnected feature that appear more fibrillar than the polymers with the odd linkages. As far as charge carrier mobility is concerned, the average number drops from 0.023 cm2 V-1 s(-1) to 7.9 X 10(-6) cm(2) V-1 s(-1) as the CBS moves from C2 to C12. It is intriguing to observe that even-numbered polymers outperform the adjacent odd-numbered polymers, despite the fact that the latter show higher ordering and crystallinity in thin films. When these polymers are mixed with fully conjugated DPP-CO (2 wt %, designated as tie chain polymer), the obtained cSPBs witness a dramatic increase (2-4 orders of magnitude) in charge carrier mobility. Interestingly, the odd even effect is not found for charge transport in the c-SPBs. This work reveals that the length of CBSs plays a significant role in charge transport properties of the matrix polymers and reconfirms that efficient charge transport properties of the c-SPB result from the interactions between matrix polymers and tie chain polymers. This begins to provide guidelines as to what spacer lengths may be utilized to offer the best balance between processing and charge transport properties.
    DOI:
    10.1021/acs.macromol.6b00050
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