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Copper;samarium | 12645-14-6

中文名称
——
中文别名
——
英文名称
Copper;samarium
英文别名
copper;samarium
Copper;samarium化学式
CAS
12645-14-6
化学式
Cu2Sm
mdl
——
分子量
277.452
InChiKey
BSTLPRXDQPBOTL-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:
    3
  • 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:
    三氢化钐 以 melt 为溶剂, 生成 Copper;samarium
    参考文献:
    名称:
    SmCu2 的低温 X 射线衍射、传输特性、比热、热膨胀和磁性研究
    摘要:
    已经研究了正交晶系 SmCu2 的各种物理特性(低温 X 射线衍射、电阻率、热导率、热电势、比热、热膨胀和磁化率)。已经观察到 J=5/2 Hund 基态的显着贡献。从热膨胀实验中获得的整体晶体场分裂的估计值为 110 K。磁熵表明双基态,因为观测值 (Sm=5.50+or-0.2 J mol-1 K-1 ) 非常接近理论 R ln 2。在电阻率和磁化率结果中可以看到 J=7/2 多重峰的额外影响。在磁振子热导率的框架内讨论了磁有序区域(尼尔温度 TN = 23 K)中热导率的显着增加。
    DOI:
    10.1088/0953-8984/2/6/008
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文献信息

  • Low-temperature X-ray diffraction, transport properties, specific-heat, thermal expansion and magnetic investigations of SmCu<sub>2</sub>
    作者:E Gratz、N Pillmayr、E Bauer、H Muller、B Barbara、M Loewenhaupt
    DOI:10.1088/0953-8984/2/6/008
    日期:1990.2.12
    variety of physical properties (low-temperature X-ray diffraction, electrical resistivity, thermal conductivity, thermopower, specific heat, thermal expansion and susceptibility) of orthorhombic SmCu2 have been studied. A significant contribution of the J=5/2 Hund ground state has been observed. An estimation of the overall crystal-field splitting obtained from the termal expansion experiment yields
    已经研究了正交晶系 SmCu2 的各种物理特性(低温 X 射线衍射、电阻率、热导率、热电势、比热、热膨胀和磁化率)。已经观察到 J=5/2 Hund 基态的显着贡献。从热膨胀实验中获得的整体晶体场分裂的估计值为 110 K。磁熵表明双基态,因为观测值 (Sm=5.50+or-0.2 J mol-1 K-1 ) 非常接近理论 R ln 2。在电阻率和磁化率结果中可以看到 J=7/2 多重峰的额外影响。在磁振子热导率的框架内讨论了磁有序区域(尼尔温度 TN = 23 K)中热导率的显着增加。
  • Changing phase equilibria: A method for microstructure optimization and properties improvement in preparing anisotropic Sm2Fe17N3 powders
    作者:Cifu Lu、Xiufeng Hong、Xiaoqian Bao、Xuexu Gao、Jie Zhu
    DOI:10.1016/j.jallcom.2019.01.098
    日期:2019.5
    Sm2Fe17N3 compound possesses excellent intrinsic permanent magnet properties. Sm2Fe17N3 is usually produced by nitridation of the Sm2Fe17 alloy; however, it is difficult to avoid the formation of alpha-Fe and SmFe3 phases in the Sm-Fe system, which may have adverse effects on the magnetic properties of the final magnets. In this study, the three-phase region of SmCu + SmCu2 +Sm2Fe17 was determined experimentally and a partial isothermal section of the Sm-Fe-Cu phase diagram at 450 degrees C was established. Based on this newly determined three-phase region, a parent alloy free of alpha-Fe and SmFe3 phases was obtained and the effects of Sm-Cu assistant phases on the microstructure and magnetic properties of nitrided powder were investigated. Anisotropic Sm2Fe17N3 powders free of alpha-Fe and having a high (BH)(max) exceeding 31 MGOe and H-cj of 13.9 kOe were obtained using a parent alloy containing 3 at.% of Sm-Cu assistant phases. The magnetization reversal process of anisotropic Sm2Fe17N3 powders with and without alpha-Fe was investigated and the underlying mechanisms were analyzed. (C) 2019 Elsevier B.V. All rights reserved.
  • Investigation of the phase diagrams of the Sm–Ni–Pb and Sm–Cu–Pb systems
    作者:L.D. Gulay
    DOI:10.1016/s0925-8388(02)00825-3
    日期:2003.1
    The phase diagrams of the Sm-Ni-Pb and Sm-Cu-Pb systems were constructed using X-ray phase analysis. Four ternary compounds SmNiPb (TiNiSi structure type, space group Pnma, a=7.3199(3) Angstrom, b=4.5769(2) Angstrom, c=7.8015(3) Angstrom), Sm2Ni2Pb (Mn2AlB2 structure type, space group Cmmm, a=4.087(1) Angstrom, b=14.187(3) Angstrom, c=3.716(1) Angstrom), Sm5NiPb3 (Hf5CuSn3 structure type, space group P6(3)/mcm, a=9.171(2) Angstrom, c=6.710(1) Angstrom) and Sm12Ni6Pb (Sm12Ni6In structure type, space group Im3, a=9.825(2) Angstrom) exist in the Sm-Ni-Pb system. Two ternary compounds SmCuPb (LiGaGe structure type, space group P6(3)mc, a=4.5965(2) Angstrom, c=7.4769(2) Angstrom) and Sm5CuPb3 (Hf5CuSn3 structure type, space group P6(3)/mcm, a=9.316(1) Angstrom, c=6.6881(4) Angstrom) exist in the Sm-Cu-Pb system. (C) 2002 Elsevier Science B.V. All rights reserved.
  • The isothermal section of the phase diagram of Sm–Cu–Mg ternary system at 670 K
    作者:Bernard Marciniak、Volodymyr Pavlyuk、Ewa Rozycka-Sokolowska、Lukasz Karwowski、Zygmunt Bak
    DOI:10.1016/j.jallcom.2015.08.183
    日期:2015.12
    The isothermal section of the Sm-Cu-Mg system at 670 K was studied in the 0-50 at.% Mg concentration range. The phase analysis was carried out by scanning electron microscopy (SEM), electron probe microanalysis (EPMA), wavelength dispersive spectrometry (WDS) and X-ray powder diffraction (XRPD) techniques. The X-ray single crystal and powder analysis were used for structure investigations. Of the nine ternary phases (tau(1)-tau(9)) which were found to exist in this section are seven new phases, tau(1) - Sm60.1Cu26.4Mg13.5, tau(3) - Sm22.5Cu74.3Mg3.2, tau(4) - SmCu4Mg, tau(5) - SmCuMg, tau(6) -SmCuMg2, tau(7) - Sm81.2Cu10.3Mg8.5 and tau(8) - Sm4Cu10Mg3, and two known phases, tau(2) - Sm2Cu2Mg and tau(9) - SmCu9Mg2. As the result of our investigation the crystal structures of tau(2), tau(4), tau 5, tau 6 and tau 8 phases have been established. Moreover, it has been found that the solubility of Mg and Cu in Sm-Cu and Sm-Mg binary phases, respectively, is insignificant, and that the maximum solubility takes place in the case of Cu2Mg phase, which dissolves up to 5 at.% Sm. (C) 2015 Elsevier B.V. All rights reserved.
  • Rotter, M.; Doerr, M.; Loewenhaupt, M., Physical Review B: Condensed Matter and Materials Physics, p. 1 - 6
    作者:Rotter, M.、Doerr, M.、Loewenhaupt, M.、Witte, U.、Svoboda, P.、et al.
    DOI:——
    日期:——
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