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Iron;lutetium | 12023-15-3

中文名称
——
中文别名
——
英文名称
Iron;lutetium
英文别名
iron;lutetium
Iron;lutetium化学式
CAS
12023-15-3
化学式
Fe2Lu
mdl
——
分子量
286.661
InChiKey
GUZVXPBOEVZXAC-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

  • 作为反应物:
    描述:
    Iron;lutetium氢气 以 neat (no solvent, solid phase) 为溶剂, 生成
    参考文献:
    名称:
    Heat capacity and thermodynamic functions of LuFe2H2.41 and ErFe2H2.41
    摘要:
    DOI:
    10.1016/0022-4596(86)90215-x
  • 作为产物:
    描述:
    参考文献:
    名称:
    高温直接合成量热法测定镧系-铁系二元金属间化合物的标准生成焓
    摘要:
    摘要 通过高温直接合成量热法在 1373 ± 2 K 下测量了一些镧系元素-铁系金属间化合物的标准生成焓。 报告了以下以 kJ/mole 原子为单位的结果: Ce 2 Fe 17 (-1.6 ± 2.8); Pr 2 Fe 17 (-0.2 ± 3.0);Nd 2 Fe 17 (-3.0 ± 2.7);Sm 2 Fe 17 (-3.1 ± 3.2);GdFe 2 (-2.4±3.0);HoFe 2 (-2.6 ± 3.3);ErFe 2 (-1.9 ± 3.0);TmFe 2 (-2.2 ± 2.8);LuFe 2 (-3.6 ± 3.1)。一些已确立技术应用的二元和三元形状记忆合金的标准形成焓也已被测量。它们是:Terfenol-D (-1.5 ± 3.1)、Samfenol (-13.6 ± 3.1)、Galfenol (-10.4 ± 2.8);Nd 2 Fe 14 B (-9.6 ±
    DOI:
    10.1016/j.jallcom.2012.11.035
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文献信息

  • The standard enthalpies of formation of some binary intermetallic compounds of lanthanide–iron systems by high temperature direct synthesis calorimetry
    作者:S.V. Meschel、P. Nash、Q.N. Gao、J.C. Wang、Y. Du
    DOI:10.1016/j.jallcom.2012.11.035
    日期:2013.3
    formation of some binary and ternary shape memory alloys, which have established technological application, have also been measured. These are: Terfenol-D (−1.5 ± 3.1), Samfenol (−13.6 ± 3.1), Galfenol (−10.4 ± 2.8); Nd 2 Fe 14 B (−9.6 ± 3.2). The values are compared with predicted values of the semiempirical model of Miedema and Coworkers and with predictions by ab initio calculations. We will present
    摘要 通过高温直接合成量热法在 1373 ± 2 K 下测量了一些镧系元素-铁系金属间化合物的标准生成焓。 报告了以下以 kJ/mole 原子为单位的结果: Ce 2 Fe 17 (-1.6 ± 2.8); Pr 2 Fe 17 (-0.2 ± 3.0);Nd 2 Fe 17 (-3.0 ± 2.7);Sm 2 Fe 17 (-3.1 ± 3.2);GdFe 2 (-2.4±3.0);HoFe 2 (-2.6 ± 3.3);ErFe 2 (-1.9 ± 3.0);TmFe 2 (-2.2 ± 2.8);LuFe 2 (-3.6 ± 3.1)。一些已确立技术应用的二元和三元形状记忆合金的标准形成焓也已被测量。它们是:Terfenol-D (-1.5 ± 3.1)、Samfenol (-13.6 ± 3.1)、Galfenol (-10.4 ± 2.8);Nd 2 Fe 14 B (-9.6 ±
  • Temperature dependence of the electrical resistivity of REFe2 compounds
    作者:E. Gratz、E. Bauer、H. Nowotny、A.T. Burkov、M.V. Vedernikov
    DOI:10.1016/0038-1098(89)90013-6
    日期:1989.3
    Abstract The temperature dependence of the electrical resistivity of the REFe 2 compounds (RE = Y, Ce, Gd, Tb, Dy, Ho, Er, Tm, Lu) in the range from 4 K up to 1000 K are presented. The outstanding feature of CeFe 2 is also demonstrated by the temperature dependence of the thermo-power. The analysis of these data reveals that the Fe 3 d moments act as localized moments. This is supported by bandstructure
    摘要 介绍了REFe 2 化合物(RE = Y、Ce、Gd、Tb、Dy、Ho、Er、Tm、Lu)在4 K 至1000 K 范围内电阻率的温度依赖性。CeFe 2 的突出特点还体现在热功率的温度依赖性上。对这些数据的分析表明,Fe 3 d 矩充当局部矩。这得到了对 YFe 2 和 LuFe 2 进行的能带结构计算的支持。
  • Local magnetic fields in ferromagnetic intermetallic compounds of cubic Laves-phase type
    作者:S. Barth、E. Albert、G. Heiduk、A. Möslang、A. Weidinger、E. Recknagel、K. H. J. Buschow
    DOI:10.1103/physrevb.33.430
    日期:——
  • Mean field exchange constants in rare-earth–Fe2 laves phase compounds
    作者:J. Ilarraz、A. Del Moral
    DOI:10.1002/pssa.2210570107
    日期:1980.1.16
  • Strain in single-crystal<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>R</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Fe</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mn /><mml:mo>(</mml:mo><mml:mn>110</mml:mn><mml:mo>)</mml:mo><mml:mn /></mml:math>thin films<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mo>(</mml:mo><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Y</mml:mi><mml:mo>,</mml:mo></mml:math>Sm, Gd, Tb,<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Dy</mml:mi></mml:mrow><mml:mrow><mml:mn>0.7</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Tb</mml:mi></mml:mrow><mml:mrow><mml:mn>0.3</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>,</mml:mo></mml:math>Dy, Er, Lu)
    作者:A. Mougin、C. Dufour、K. Dumesnil、N. Maloufi、Ph. Mangin、G. Patrat
    DOI:10.1103/physrevb.59.5950
    日期:——
    Single-crystalline RFe2(110) compounds (R = Y, Sm, Gd, Tb, Dy0.7Tb0.3, py, Fr, and Lu) have been grown by molecular-beam epitaxy. Compared to the bulk compounds, the chin films exhibit modifications of the magnetic anisotropy, related tb the strains induced during deposition. We present here a detailed determination of in-plane and out-of-plane parameters using x-ray and neutron diffraction. RFe2 films and RFe2 /YFe2 bilayers have been deposited on a Nb buffer covered with Fe. Both systems are strained compared to bulk compounds: they are expanded in the plane of epitaxy and compressed along the growth direction. For single RFe2 films, the strains do not depend, on the lattice parameters of the corresponding bulk compounds, i.e., on the large mismatch between the film and the buffer (around 10%). The sign and the values of the strains are explained with a model of differential thermal contraction between the film and the substrate. For RFe2 films involved in RFe2/YFe2 bilayers, the mismatch between RFe2, and the YFe2, layer is smaller and the strains in the RFe2 films do depend on the bulk lattice parameters. Their evolution can be explained with an elastic model. [S0163-1829(99)00107-1].
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