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5-azido-5-(3,5-di-tert-butylbenzyl)pyrimidine-2,4,6(1H,3H,5H)-trione | 1245570-48-2

中文名称
——
中文别名
——
英文名称
5-azido-5-(3,5-di-tert-butylbenzyl)pyrimidine-2,4,6(1H,3H,5H)-trione
英文别名
5-Azido-5-[(3,5-ditert-butylphenyl)methyl]-1,3-diazinane-2,4,6-trione
5-azido-5-(3,5-di-tert-butylbenzyl)pyrimidine-2,4,6(1H,3H,5H)-trione化学式
CAS
1245570-48-2
化学式
C19H25N5O3
mdl
——
分子量
371.439
InChiKey
AVDFNLMYGWRBLI-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):
    5.2
  • 重原子数:
    27
  • 可旋转键数:
    5
  • 环数:
    2.0
  • sp3杂化的碳原子比例:
    0.53
  • 拓扑面积:
    89.6
  • 氢给体数:
    2
  • 氢受体数:
    5

反应信息

  • 作为反应物:
    描述:
    5-azido-5-(3,5-di-tert-butylbenzyl)pyrimidine-2,4,6(1H,3H,5H)-trione足球烯氯苯 为溶剂, 反应 48.0h, 以37%的产率得到
    参考文献:
    名称:
    Self-Assembly of Supramolecular Fullerene Ribbons via Hydrogen-Bonding Interactions and Their Impact on Fullerene Electronic Interactions and Charge Carrier Mobility
    摘要:
    The anisotropy of the electronic interactions between fullerenes in crystalline solids was examined using a confocal fluorescence microscope by probing the polarization of the fluorescence emission arising from fullerene excimer-like emitting states. Crystals of Can obtained by vacuum-sublimation or from chloroform solution exhibited no or little polarization (p = 0 or 0.11, respectively), as expected from the high symmetry of the C-60 fcc lattice or the low degree of anisotropy induced by included solvent molecules. The use of hydrogen-bonding to supramolecularly control interfullerene electronic interactions was explored using a fullerene derivative (1) combining a solubilizing 3,4-di-tert-butylbenzene group and a barbituric acid hydrogen-bonding (H-B) moiety. The crystal structure of 1 establishes the existence of fullerene H-B tapes along which interfullerene electronic interactions are expected to be large. In agreement with this, we observe very strong polarization of the fullerene excimer-like emission (p = 0.78), indicative of a high degree of anisotropy in the fullerene interactions. The charge-carrier mobility of 1 as determined from OFET devices was found to be lower than that of C-60 (1.2 x 10(-4) vs 1.2 x 10(-2) cm(2)/s V), which is rationalized on the basis of the reduced dimensionality of 1 as a wire-like semiconductor and variations in the morphology of the device active layer revealed by AFM measurments.
    DOI:
    10.1021/ja104750f
  • 作为产物:
    描述:
    5-(3,5-di-tert-butylbenzyl)pyrimidine-2,4,6(1H,3H,5H)-trione 在 N-溴代丁二酰亚胺(NBS) 、 sodium azide 作用下, 以 N,N-二甲基甲酰胺 为溶剂, 反应 4.0h, 以92%的产率得到5-azido-5-(3,5-di-tert-butylbenzyl)pyrimidine-2,4,6(1H,3H,5H)-trione
    参考文献:
    名称:
    Self-Assembly of Supramolecular Fullerene Ribbons via Hydrogen-Bonding Interactions and Their Impact on Fullerene Electronic Interactions and Charge Carrier Mobility
    摘要:
    The anisotropy of the electronic interactions between fullerenes in crystalline solids was examined using a confocal fluorescence microscope by probing the polarization of the fluorescence emission arising from fullerene excimer-like emitting states. Crystals of Can obtained by vacuum-sublimation or from chloroform solution exhibited no or little polarization (p = 0 or 0.11, respectively), as expected from the high symmetry of the C-60 fcc lattice or the low degree of anisotropy induced by included solvent molecules. The use of hydrogen-bonding to supramolecularly control interfullerene electronic interactions was explored using a fullerene derivative (1) combining a solubilizing 3,4-di-tert-butylbenzene group and a barbituric acid hydrogen-bonding (H-B) moiety. The crystal structure of 1 establishes the existence of fullerene H-B tapes along which interfullerene electronic interactions are expected to be large. In agreement with this, we observe very strong polarization of the fullerene excimer-like emission (p = 0.78), indicative of a high degree of anisotropy in the fullerene interactions. The charge-carrier mobility of 1 as determined from OFET devices was found to be lower than that of C-60 (1.2 x 10(-4) vs 1.2 x 10(-2) cm(2)/s V), which is rationalized on the basis of the reduced dimensionality of 1 as a wire-like semiconductor and variations in the morphology of the device active layer revealed by AFM measurments.
    DOI:
    10.1021/ja104750f
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