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dinitrogen

中文名称
——
中文别名
——
英文名称
dinitrogen
英文别名
azane
dinitrogen化学式
CAS
——
化学式
N2
mdl
——
分子量
30.0
InChiKey
XKMRRTOUMJRJIA-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):
    0.32
  • 重原子数:
    2
  • 可旋转键数:
    0
  • 环数:
    0.0
  • sp3杂化的碳原子比例:
    0.0
  • 拓扑面积:
    2
  • 氢给体数:
    2
  • 氢受体数:
    2

反应信息

  • 作为反应物:
    描述:
    5-bromo-4-chloro-7<(2-hydroxyethoxy)methyl>pyrrolo<2,3-d>pyrimidinedinitrogen 在 silica gel 、 甲醇氯仿 作用下, 以 甲醇 为溶剂, 反应 10.0h, 以to afford 11, 0.18 g (31.25%), mp 163-164 degrees C的产率得到4-氨基-5-溴-7-(2-羟基乙氧基甲基)吡咯并(2,3-d)嘧啶
    参考文献:
    名称:
    Acyclic pyrrolo[2,3-D]pyrimidine analogs as antiviral agents
    摘要:
    公开号:
    US04927830A1
  • 作为产物:
    描述:
    nitrogen 以 gas 为溶剂, 生成 dinitrogen
    参考文献:
    名称:
    亚稳态N 2簇离子的定量顺序衰减序列(N 2)n + * →(N 2)n -1 + * →…→N 2 +
    摘要:
    首次实验观察到了亚稳态分子簇离子的顺序衰减。N 2团簇离子是通过超音速N 2团簇束的电子碰撞电离产生的,并通过双聚焦扇形场质谱仪(反向几何结构)进行分析。发现亚稳态的N 2簇离子在微秒时间范围内会损失一个以上的N 2分子,并且主要通过连续序列(N 2)n + * →(N 2)n -1 + * →…→N 2 +衰变。在每个连续的衰变步骤中蒸发单个单体。亚稳衰变率详细群集确定大小2⩽ Ñ ⩽6和Ñ = 20介于1个10之间6小号-1和后离子形成所经过的时间强烈地依赖。衰减率显示出准周期模式,与以下假设一致:在采样时间内,多达四个振动量子(存储在群集中的中性N 2分子中)松弛进入群集的声子池。
    DOI:
    10.1016/0009-2614(88)87193-8
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文献信息

  • 2-Oxo-Piperidinyl Derivatives
    申请人:UCB Pharma, S.A.
    公开号:US20150011526A1
    公开(公告)日:2015-01-08
    The present invention relates to 2-oxo-piperidinyl derivatives, processes for preparing them, pharmaceutical compositions containing them and their use as pharmaceuticals.
    本发明涉及2-氧代哌啶基衍生物、其制备过程、含有它们的制药组合物以及它们作为药物的用途。
  • 2-oxo-piperidinyl derivatives
    申请人:UCB Pharma, S.A.
    公开号:US09067930B2
    公开(公告)日:2015-06-30
    The present invention relates to 2-oxo-piperidinyl derivatives, processes for preparing them, pharmaceutical compositions containing them and their use as pharmaceuticals.
    本发明涉及2-氧代哌啶基衍生物,其制备方法,含有它们的药物组合物以及它们作为药物的用途。
  • Structural and mechanical properties of (B<sub>0.5−<i>x</i></sub>Si<sub><i>x</i></sub>)N<sub>0.5</sub>films synthesized by dual‐ion‐beam deposition
    作者:C. W. Ong、X.‐A. Zhao、Y. M. Ng、K. F. Chan、T. C. Tsang、C. L. Choy、P. W. Chan
    DOI:10.1063/1.117225
    日期:1996.12.2
    The structural and mechanical properties of ionbeam deposited (B0.5−xSix)N0.5 films (0≤x≤0.5) were characterized by x‐ray photoelectron spectroscopy, infrared absorption experiments, and nanoindentation tests. A single‐layer BN film (x=0) has 70 vol. % in cubic phase (c‐BN), and a hardness of 38 GPa. However, it peeled off very soon after deposition due to the high internal stress. If a buffer layer
    通过X射线光电子能谱、红外吸收实验和纳米压痕测试表征了离子束沉积的(B0.5-xSix)N0.5薄膜(0≤x≤0.5)的结构和机械性能。单层 BN 膜 (x=0) 具有 70 vol. 立方相 (c-BN) 中的 %,硬度为 38 GPa。然而,由于高内应力,它在沉积后很快剥落。如果首先沉积缓冲层,然后是 (B0.5-xSix)N0.5 薄膜,x≊0.013,则整个配置非常牢固地粘附在石英和硅基板上。这种粘附力的提高可能是由于形成了 Si-N 键,这部分地释放了 (B0.5-xSix)N0.5 薄膜内部的应力。由于Si含量低,膜结构保持高度立方,并且没有可观察到的硬度下降。对于更高的 x,(B0.5-xSix)N0.5 薄膜中的立方结构迅速消失,取而代之的是六方结构。这种结构变化导致硬度从 38 迅速下降到 12 ...
  • Amide from Dinitrogen by In Situ Cleavage and Partial Hydrogenation Promoted by a Transient Zero-Valent Thorium Synthon
    作者:Ilia Korobkov、Sandro Gambarotta、Glenn P. A. Yap
    DOI:10.1002/anie.200352205
    日期:2003.10.20
  • Rotational spectroscopy and molecular structure of 15N2–14N2O
    作者:Helen O. Leung
    DOI:10.1063/1.478321
    日期:1999.3.1
    The rotational spectrum of 15N2–14N2O has been recorded in the 7–19 GHz region with a pulsedmolecular beam,Fourier transformmicrowavespectrometer. An internal motion of the 15N2 subunit has been observed and the nuclear quadrupole hyperfine structurein each internal motion state has been analyzed using the WatsonS-reduced Hamiltonian with the inclusion of nuclear quadrupole couplinginteractions. The spectroscopic constants of the ground internal motion state are not welldetermined since only 4 transitions have been observed, but they are similar to those ofthe excited internal motion state that are determined from the analysis of 14a- and b-type transitions. The rotational andcentrifugal distortion constants (in MHz) for the excited internal motion state areA=12 791.307 0(2),B=2 014.982 4(1),C=1 728.950 45(7),DJ=1.052 5(2)×10−2,DJK=3.933 7(3)×10−1,d1=−1.822(3)×10−3,d2=−1.118(6)×10−3. The nuclear quadrupole coupling constants (in MHz) in the excitedinternal motion state for the terminal 14N nucleus in N2O are χaa=0.3465(4),χbb=−0.7445(5), and χcc=0.3980(5), while those for the central 14N nucleus are χaa=0.1023(9),χbb=−0.2528(8), and χcc=0.1505(8). These spectroscopic constants are consistent with aT-shaped structure, with 15N2 forming the leg of the T. The intermolecular distance is3.691 Å. The 15N2 axis and the 14N2O axis make an angle of 13° and 81° with the intermolecularaxis, respectively. The nuclear quadrupole coupling constants show electric field gradient perturbationin the N2O subunit, with the field gradient at the central nitrogenaffected to a greater extent than that at the terminal nitrogen. This perturbation islikely due to electron charge redistribution in N2O upon complexation with N2.
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