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divanadium | 12597-60-3

中文名称
——
中文别名
——
英文名称
divanadium
英文别名
vanadium cluster;vanadium dimer;vanadium
divanadium化学式
CAS
12597-60-3
化学式
V2
mdl
——
分子量
101.883
InChiKey
GPPXJZIENCGNKB-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):
    -0.01
  • 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

  • 作为反应物:
    描述:
    divanadium 在 benzene 作用下, 以 neat (no solvent) 为溶剂, 生成 单苯钒
    参考文献:
    名称:
    芳烃-金属二聚体配合物,双(苯)钒[(C6H6)2V2]和苯钒[[C6H6)V2];实验和x.alpha。理论。3
    摘要:
    DOI:
    10.1021/j100398a010
  • 作为产物:
    描述:
    以 gaseous matrix 为溶剂, 生成 divanadium
    参考文献:
    名称:
    Dititanium and divanadium
    摘要:
    The Ar+ laser-excited spectrum of matrix-isolated V2 consists of a resonance Raman progression with ωe=537.5 cm−1 and ωexe=4.2 cm−1. With increasing laser power several members of an anti-Stokes progression and sequence components on both Stokes and anti-Stokes members of this progression were observed and attributed to transitions originating from vibrationally excited stated populated as a result of laser irradiation. A second system with ωe=508 and ωexe=3.3 cm−1 also grew in with increasing laser power and 496.5 nm excitation. This was interpreted as a resonance Raman progression within an electronically excited state (A) of V2. The electronic resonance Raman spectrum corresponding to the A→X transition was also observed as well as one to another low-lying electronic excited state. The v′=0 level of state A was found to lie 1860 cm−1 above the v″=0 level of the ground state. The multiple photon nature of the transitions discussed above was determined by performing laser power measurements. The resonance Raman spectrum of Ti2 was excited with HeNe and dye laser illumination in solid argon matrices containing titanium. As with V2, laser irradiation populated excited vibrational states of the ground state, producing an anti-stokes, resonance Raman progression. Isotopic components of Ti2 were resolvable under high resolution, corroborating the assignment. A discussion of multiple bonding in transition metal dimers is presented which shows that the contribution of bonds originating from the atomic d orbitals do not always contribute uniformly to the metal–metal force constant. Hence the formal bond order is not always a good gauge of the bond strength of a transition metal dimer.
    DOI:
    10.1063/1.440143
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文献信息

  • Irion, Manfred P.; Schnabel, P.; Selinger, Adrian, Berichte der Bunsen-Gesellschaft, <hi>1990</hi>, vol. 94, # 11, p. 1291 - 1295
    作者:Irion, Manfred P.、Schnabel, P.、Selinger, Adrian
    DOI:——
    日期:——
  • Arene-metal dimer complexes, bis(benzene)vanadium [(C6H6)2V2] and benzenevanadium [(C6H6)V2]; experiment and x.alpha. theory. 3
    作者:Mark P. Andrews、Geoffrey A. Ozin
    DOI:10.1021/j100398a010
    日期:1986.3
  • Dititanium and divanadium
    作者:C. Cossé、M. Fouassier、T. Mejean、M. Tranquille、D. P. DiLella、M. Moskovits
    DOI:10.1063/1.440143
    日期:1980.12.15
    The Ar+ laser-excited spectrum of matrix-isolated V2 consists of a resonance Raman progression with ωe=537.5 cm−1 and ωexe=4.2 cm−1. With increasing laser power several members of an anti-Stokes progression and sequence components on both Stokes and anti-Stokes members of this progression were observed and attributed to transitions originating from vibrationally excited stated populated as a result of laser irradiation. A second system with ωe=508 and ωexe=3.3 cm−1 also grew in with increasing laser power and 496.5 nm excitation. This was interpreted as a resonance Raman progression within an electronically excited state (A) of V2. The electronic resonance Raman spectrum corresponding to the A→X transition was also observed as well as one to another low-lying electronic excited state. The v′=0 level of state A was found to lie 1860 cm−1 above the v″=0 level of the ground state. The multiple photon nature of the transitions discussed above was determined by performing laser power measurements. The resonance Raman spectrum of Ti2 was excited with HeNe and dye laser illumination in solid argon matrices containing titanium. As with V2, laser irradiation populated excited vibrational states of the ground state, producing an anti-stokes, resonance Raman progression. Isotopic components of Ti2 were resolvable under high resolution, corroborating the assignment. A discussion of multiple bonding in transition metal dimers is presented which shows that the contribution of bonds originating from the atomic d orbitals do not always contribute uniformly to the metal–metal force constant. Hence the formal bond order is not always a good gauge of the bond strength of a transition metal dimer.
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