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titanium(2+);chloride | 21879-29-8

中文名称
——
中文别名
——
英文名称
titanium(2+);chloride
英文别名
——
titanium(2+);chloride化学式
CAS
21879-29-8
化学式
ClTi
mdl
——
分子量
83.333
InChiKey
ZNFNVLRXFXNGOK-UHFFFAOYSA-M
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):
    0.69
  • 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:
    0
  • 氢给体数:
    0
  • 氢受体数:
    0

反应信息

  • 作为产物:
    描述:
    四氯化钛 以 gaseous matrix 为溶剂, 生成 titanium(2+);chloride
    参考文献:
    名称:
    A spectrum of TiCl+ in the yellow-green
    摘要:
    DOI:
    10.1016/0022-2852(90)90062-u
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文献信息

  • A spectrum of TiCl+ in the yellow-green
    作者:Walter J. Balfour、K.S. Chandrasekhar
    DOI:10.1016/0022-2852(90)90062-u
    日期:1990.2
  • Laser velocity modulation spectroscopy of TiCl+: Observation of the A 3Δ(3d2) state and deperturbation of the X 3Φ−A 3Δ complex
    作者:C. Focsa、B. Pinchemel、J.-L. Féménias、T. R. Huet
    DOI:10.1063/1.475313
    日期:1997.12.22
    A single mode cw dye laser along with velocity modulation was used to record weak bands of TiCl+ in the spectral region 17 100–18 600 cm−1. The ions were produced in the positive column of an ac glow discharge with a gas mixture of He/TiCl4. These new bands have been identified as linking the upper already known [17.8]3Δ(3d4s) state to respectively the X 3Φ(v=1) state and to a newly observed A 3Δ(v=0) state located 350 cm−1 above the X 3Φ(v=0) state. As suggested by Focsa et al. (J. Chem. Phys. 106, 9044 (1997)) the A 3Δ(3d2) state was found to be responsible for the perturbations observed in the X 3Φ(3d2) state. The spin-orbit components of the A 3Δ(v=0) and the X 3Φ(v=1) states revealed interaction leading to homogeneous and heterogeneous perturbations. A set of deperturbed parameters has been determined with the help of a full matrix-based handling of the A 3Δ(v=0) and the X 3Φ(v=0,1) states. Study of the contributions of the basis functions to the eigenvectors of the diagonalized matrix displayed evidence of a reversal of the leading character of the Ω=3 spin-orbit components of the A 3Δ(v=0) and the X 3Φ(v=1) states. A remarkable example of avoided crossing has been observed between the A 3Δ1(v=0) and the X 3Φ2(v=1) spin-orbit components.
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