terbium phosphide

• 分子结构分类: 无机化合物 - 混合金属/非金属化合物 - 各种混合金属/非金属
• 英文名称: terbium phosphide
• 英文别名: terbium monophosphide；Phosphane;terbium；phosphane;terbium
• 化学式: PTb
• 分子量: 189.899
• InChiKey: OPNMSGJNDOUIOZ-UHFFFAOYSA-N

计算性质

• 辛醇/水分配系数(LogP)：
  0.06
• 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：

  锰 、 铜 、 磷化氢 、 terbium phosphide 反应 240.0h， 生成 terbium manganese copper phosphide
  参考文献：
  名称：

  Rare-Earth Manganese Copper Phosphides REMnCu₄P₃ (RE = Gd–Ho): The First Quaternary Ordered Variants of the YCo₅P₃-Type Structure

  摘要：

  The quaternary rare-earth phosphides REMnCu4P3 (RE = Gd-Ho) were obtained from direct reactions of the elements at 800 degrees C. They are the first examples in which ordering of two different transition-metal atoms takes place within the orthorhombic YCo5P3-type structure [Pearson symbol oP36, space group Pnma, Z = 4; a = 12.667(2)-12.6489(4) angstrom, b = 3.8119(7)-3.7755(1) angstrom, and c = 10.895(2)-10.8632(4) angstrom for RE = Gd-Ho]. Columns of trigonal prisms centered by P atoms are connected in propellor-shaped units in zigzag arrangements to generate square-pyramidal (CN5) sites that are occupied by Mn atoms and tetrahedral sites (CN4) that are occupied by Cu atoms. Spin-polarized band-structure calculations predict that the hypothetical compound YMnCu4P3 will exhibit magnetic ordering. Electrical resistivity measurements on TbMnCu4P3 indicate a poor metal.

  DOI：

  10.1021/ic502075x
• 作为产物：
  描述：

  氢化铽 、 phosphorous 以 neat (no solvent) 为溶剂， 生成 terbium phosphide
  参考文献：
  名称：

  Phase transitions of lanthanide monophosphides with NaCl-type structure at high pressures

  摘要：

  Lanthanide monophosphides LnP (Ln = La, Ce, Pr, Nd, Sm, Gd, To, Tm and Yb) with a NaCl-type structure have systematically been prepared at high temperatures. Using synchrotron radiation, X-ray diffractions of LnP have been studied up to 61 GPa at room temperature. The NaCl-CsCl transition for CeP is found at around 25 GPa. First-order phase transitions of LnP (Ln = La, Pr and Nd) with the crystallographic change occur at around 24, 26 and 30 GPa, respectively. The structure of the high pressure phases of these phosphides is a body center tetragonal structure (Ln: 0, 0, 0; P: 1/2, 1/2, 1/2; space group P4/mmm), which can be seen as the distorted CsCl-type structure. The Pr-P distance in the high pressure form of PrP is 2.789 Angstrom. This almost agrees with the sum of covalent radii of Pr and P The Pr-P bond has the covalent character at very high pressures. Similar results are also obtained for LaP and NdP. The pressure-induced phase transitions of SmP, GdP, TbP, TmP and YbP occur at around 35, 40, 38, 53 and 51 GPa, respectively. The structure of the high pressure phase is unknown. The phase transitions of LnP with many f-electrons are not due to the mechanism of the ordinary NaCl-CsCl transition. The transition pressures of LnP increase with decreasing the lattice constants in the NaCl-type structure, which decrease with increasing atomic number of the lanthanide atoms. (C) 1998 Elsevier Science B.V.

  DOI：

  10.1016/s0375-9601(98)00840-8