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nitric oxide | 51006-61-2

中文名称
——
中文别名
——
英文名称
nitric oxide
英文别名
——
nitric oxide化学式
CAS
51006-61-2
化学式
Ar*NO
mdl
——
分子量
69.9541
InChiKey
FUOSJNNMZMSGAZ-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):
    -0.45
  • 重原子数:
    3.0
  • 可旋转键数:
    0.0
  • 环数:
    0.0
  • sp3杂化的碳原子比例:
    0.0
  • 拓扑面积:
    39.37
  • 氢给体数:
    0.0
  • 氢受体数:
    1.0

反应信息

  • 作为产物:
    描述:
    氧化亚氮 以 gas 为溶剂, 生成 nitric oxide
    参考文献:
    名称:
    Product state and kinetic energy distributions in the ultraviolet photodissociation of the NO–Ar van der Waals molecule
    摘要:
    The internal state and kinetic energy distributions of the X̃ NO fragments formed from the ultraviolet photodissociation of the NO–Ar van der Waals species were obtained by laser-excited fluorescence techniques. The initially excited à NO–Ar rapidly dissociates to form X̃ NO with little rotational excitation, with vibrational excitation determined by a Franck–Condon process, with a cos2 θ angular flux distribution (θ defined relative to the direction of polarization of the pump laser), and with a speed v∼4.4×105 cm/s.
    DOI:
    10.1063/1.448896
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文献信息

  • The direct photodissociation of the van der Waals molecule NO–Ar
    作者:Patrick R. R. Langridge‐Smith、Edwin Carrasquillo M.、Donald H. Levy
    DOI:10.1063/1.440992
    日期:1981.6
    Fluoresence spectra, due to dye laser excitation, are obtained for NO–Ar. (AIP)
  • The Ã 2Σ+ state of Ar⋅NO studied using resonance-enhanced multiphoton and zero-kinetic-energy pulsed-field ionization spectroscopy
    作者:Andrew M. Bush、John M. Dyke、Paul Mack、David M. Smith、Timothy G. Wright
    DOI:10.1063/1.475402
    日期:1998.1.8
    Resonance-enhanced multiphoton ionization (REMPI) and zero-kinetic-energy pulsed-field ionization (ZEKE-PFI) techniques have been used to study the spectroscopy of the Ã 2Σ+ state of Ar⋅NO. Ã 2Σ+–X̃ 2Π REMPI spectra of Ar⋅NO have been interpreted using two different models that have allowed assignment of the observed rovibronic transitions to be made and an estimate of the strength of the à state intermolecular potential to be determined. Simulations of the spectra have indicated that the ground vibrationless level of the à state has a linear geometry while some higher vibrational levels have a skewed T-shaped structure. The analysis has also confirmed that the à state of Ar⋅NO is very weakly bound and is non-Rydberg in character. Reported for the first time are ZEKE-PFI spectra observed via the intermediate Ã 2Σ+ state. No structure was detected close to the ionization threshold, although peaks observed at higher excitation energy have been assigned to transitions to high-lying vibrational levels of the Ar⋅NO+ ion. ZEKE-PFI spectra recorded via the ground vibrational level of the intermediate à state, which has a linear structure, show progressions which correlate with transitions to highly excited van der Waals stretching and bending levels; however, spectra recorded via an intermediate level with a T-shaped geometry show progressions which correlate principally with the van der Waals stretching mode. These assignments have been interpreted in terms of the large changes in intermolecular bond length and bond angle upon ionization and fully support the interpretation of the REMPI spectra. The results of the REMPI and ZEKE-PFI spectra have also been used to investigate the character of the à state and the geometry that the complex adopts in each of the vibronic levels of this state has been rationalized in terms of the possible interactions involved.
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