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| 141312-15-4

中文名称
——
中文别名
——
英文名称
——
英文别名
——
化学式
CAS
141312-15-4
化学式
H2Si
mdl
——
分子量
32.0855
InChiKey
SYWMLUYLILUMRO-DICFDUPASA-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):
    -0.92
  • 重原子数:
    1.0
  • 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:
    0.0
  • 氢给体数:
    0.0
  • 氢受体数:
    0.0

反应信息

  • 作为反应物:
    描述:
    硅烷 以 neat (no solvent) 为溶剂, 生成 、 、
    参考文献:
    名称:
    Sequential reactions of SiD+2 with SiD4
    摘要:
    The thermal (300 K) reaction of SiD+2 with SiD4 proceeds at greater than the Langevin collision rate (21±3×10−10 cm3/molecule s ). The reaction products SiD+3, Si2D+2, and Si2D+4 are produced in a 54:7:39 ratio. Both silicon isotope exchange and adduct (Si2D+6) formation are <1% of the collision rate at silane pressures of 1–4×10−7 Torr. The branching ratio for SiD+3 formation increases with increasing internal energy of SiD+2. Sequential reactions of SiD+3 and Si2D+2 with SiD4 have been previously found to produce terminal species containing five silicon atoms. Si2D+4 reacts with SiD4 only by silicon isotope exchange at 2.0±0.7% of the collision rate (0.20±0.07×10−10 cm3/molecule s ) with no evidence of other reactions (<0.5% of the collision rate). Reaction of SiD+2 with SiD4 does not lead to unconstrained clustering and particle formation in silane plasmas. High level ab initio calculations on this system are reported by Raghavachari in his companion paper. Energies of the critical intermediates and transition states along the reaction surface are compared quantitatively to the experimental results via phase space calculations. The energies agree to within 6 kcal/mol.
    DOI:
    10.1063/1.462834
  • 作为产物:
    描述:
    硅烷乙烷-d6 以 gaseous matrix 为溶剂, 生成 、 、
    参考文献:
    名称:
    Boo; Armentrout, Journal of the American Chemical Society, 1991, vol. 113, # 18, p. 6401 - 6408
    摘要:
    DOI:
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