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硫化铌 | 12164-38-4

中文名称
硫化铌
中文别名
——
英文名称
niobium monosulfide
英文别名
Niobium sulfide (NbS);sulfanylideneniobium
硫化铌化学式
CAS
12164-38-4;39290-91-0
化学式
NbS
mdl
——
分子量
124.972
InChiKey
NYPFJVOIAWPAAV-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):
    0.65
  • 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:
    32.1
  • 氢给体数:
    0
  • 氢受体数:
    1

SDS

SDS:5cdb4b761a902bb840337a9e79b09615
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反应信息

  • 作为产物:
    描述:
    参考文献:
    名称:
    First laboratory observation of niobium monosulphide in the gas phase
    摘要:
    The diatomic molecule NbS has been observed for the first time by laser-induced fluorescence at low resolution in a supersonic molecular beam following expansion of a CS2/He (1:100) mixture through a laser-produced plasma of niobium atoms. Two band systems have been observed in the visible (400–700 nm); a strong one and a weaker one. The strong one has its origin near 15 670 cm−1 and is shown to belong to the C 4Σ−–X 4Σ− system. The weaker one has its origin likely at 15 215 cm−1 and is attributed to the 2Σ+–X 4Σ−1/2 system. The latter system is observed owing to the 2Σ+(σ1δ2)∼C4Σ−1/2 (δ2σ*1) perturbation induced by the spin–orbit operators. This perturbation has been characterized through vibrational energy shifts, vibronic lifetimes, and analysis of the perturbation matrix elements. This enables direct determination of the large second-order spin–orbit splittings in the C 4Σ− and X 4Σ− states. In the ground state, the splitting which is due to the isoconfigurational 〈2Σ+‖Hso‖X 4Σ−〉 interaction element has been established to be 63 cm−1 and is independent of the vibrational energy content. In the C state, the spin–orbit splitting arises from two interactions; one due to the isoconfigurational 〈2Σ+‖Hso‖C 4Σ−〉 interaction and the other to the 〈2Σ−(σ1δ2), (v+1)‖Hso‖C 4Σ−(δ2σ*1),v〉 interaction. The former interaction splits the C 4Σ−3/2 and C 4Σ−1/2 components by about 63 cm−1, as in the ground X 4Σ− state again independent of the vibrational energy content. The second interaction which becomes negligible at v(C 4Σ−)≥4 shifts the C 4Σ− (v=0,1,2,3) levels to lower wave numbers by 18, 15, 11, and 5 cm−1, respectively. From a Franck–Condon analysis, the electronic part of the molecular matrix elements 〈2Σ+(σ1δ2), v′‖Hso‖C 4Σ−(δ2σ1*),v″〉 is estimated to be 57 cm−1. Other molecular parameters such as vibrational frequencies and anharmonicities, radiative lifetimes, Franck–Condon factors, mixing coefficients, and approximate bond lengths are reported and discussed.
    DOI:
    10.1063/1.458240
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