Gallium--iron (4/3) | 53237-41-5

• 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: Gallium--iron (4/3)
• 英文别名: gallane;iron
• CAS: 53237-41-5
• 化学式: Fe₃Ga₄
• 分子量: 446.433
• InChiKey: HCABDUUDRHNEKV-UHFFFAOYSA-N

计算性质

• 辛醇/水分配系数(LogP)：
  -4.74
• 重原子数：
  7
• 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：

  氢化镓 、 铁粉 以 melt 为溶剂， 生成 Gallium--iron (4/3)
  参考文献：
  名称：

  通过磁化和磁阻等温线揭示流动的 Fe3Ga4 的弱停滞和场驱动的一级磁相变

  摘要：

  摘要 报道了络合物3 d 电子基Fe 3 Ga 4 的详细磁学研究。它分别在 380 和 70 K 左右经历顺磁到反铁磁 (TN) 和反铁磁到铁磁 (TC) 的转变。场冷却 (FCC) 和场冷却变暖 (FCW) 的热滞后暗示居里以下的一阶相变温度。通过探索类似逮捕的一阶现象，建议铁磁相和反铁磁相的弱相共存。在中间温度范围内，证实了从反铁磁相到铁磁相的场驱动变磁转变。进一步使系统非常接近 TN ，场引起的跃迁消失并且在 TN 之上主要顺磁贡献是明显的。

  DOI：

  10.1016/j.jmmm.2016.08.079

文献信息

• Crystal Growth, Transport, and the Structural and Magnetic Properties of Ln₄FeGa₁₂ with Ln = Y, Tb, Dy, Ho, and Er
  作者：Brenton L. Drake、Fernande Grandjean、Michael J. Kangas、Edem K. Okudzeto、Amar B. Karki、Moulay T. Sougrati、David P. Young、Gary J. Long、Julia Y. Chan

  DOI：10.1021/ic9013202

  日期：2010.1.18

  cuboctahedra of the Au3Cu type. Er4Fe0.67Ga12 is iron-deficient, leading to a distortion of the octahedral and cuboctahedral environments due to the splitting of the Ga2 site into Ga2 and Ga3 sites. Further, interstitial octahedral sites that are unoccupied in Ln4FeGa12 (Ln = Y, Tb, Dy, and Ho) are partially occupied by Fe2. Y4FeGa12 exhibits weak itinerant ferromagnetism below 36 K. In contrast, Tb4FeGa12

  LN 4 FEGA 12，其中Ln为Y，Tb时，镝，钬，和Er，通过助熔剂生长制备，结晶与立方ÿ 4的PdGa 12结构与进出口3米的空间群，并用一个= 8.5650（4），8.5610 （4），8.5350（3），8.5080（3）和8.4760（3）Å。晶体结构由铁镓八面体和面共享的Au 3 Cu型稀土立方八面体组成。尔4的Fe 0.67镓12是缺铁的，由于将Ga2位点分为Ga2和Ga3位点，导致八面体和立方八面体环境变形。此外，在Ln 4 FeGa 12中未被占据的间隙八面体位点（Ln = Y，Tb，Dy和Ho）被Fe2部分占据。Y 4 FeGa 12在36 K以下显示弱的迭代铁磁。相反，Tb 4 FeGa 12，Dy 4 FeGa 12，Ho 4 FeGa 12和Er 4 Fe 0.67 Ga 12在26、18.5、9和6 K时的摩尔磁化率具有最大的反铁磁顺序。所有化合物均表现出金属电阻率，在4
• Weak arrest-like and field-driven first order magnetic phase transitions of itinerant Fe3Ga4 revealed by magnetization and magnetoresistance isotherms
  作者：S. Shanmukharao Samatham、K.G. Suresh

  DOI：10.1016/j.jmmm.2016.08.079

  日期：2017.1

  Abstract The detailed magnetic study of complex 3 d -electron based Fe 3 Ga 4 is reported. It undergoes paramagnetic to antiferromagnetic ( T N ) and antiferromagnetic to ferromagnetic ( T C ) transitions respectively around 380 and 70 K. The thermal hysteresis of field-cooled cooling (FCC) and field-cooled warming (FCW) hints at first order phase transition below Curie temperature. A weak phase coexistence

  摘要 报道了络合物3 d 电子基Fe 3 Ga 4 的详细磁学研究。它分别在 380 和 70 K 左右经历顺磁到反铁磁 (TN) 和反铁磁到铁磁 (TC) 的转变。场冷却 (FCC) 和场冷却变暖 (FCW) 的热滞后暗示居里以下的一阶相变温度。通过探索类似逮捕的一阶现象，建议铁磁相和反铁磁相的弱相共存。在中间温度范围内，证实了从反铁磁相到铁磁相的场驱动变磁转变。进一步使系统非常接近 TN ，场引起的跃迁消失并且在 TN 之上主要顺磁贡献是明显的。
• Helical spin ordering in room-temperature metallic antiferromagnet Fe3Ga4
  作者：Brandon Wilfong、Adrian Fedorko、Danil R. Baigutlin、Olga N. Miroshkina、Xiuquan Zhou、Gregory M. Stephen、Adam L. Friedman、Vaibhav Sharma、Omar Bishop、Radhika Barua、Steven P. Bennett、Duck Young Chung、Mercouri G. Kanatzidis、Vasiliy D. Buchelnikov、Vladimir V. Sokolovskiy、Bernardo Barbiellini、Arun Bansil、Don Heiman、Michelle E. Jamer

  DOI：10.1016/j.jallcom.2022.165532

  日期：2022.10

  Metallic Fe3Ga4 displays a complex magnetic phase diagram that supports an intermediate antiferromagnetic (AFM) helical spin structure (HSS) state at room temperature which lies between two ferromagnetic (FM) phases. Magnetic measurements along the three crystallographic axes were performed in order to develop a model for the temperature and field dependence of the HSS state. These results show that

  金属 Fe 3 Ga 4显示了一个复杂的磁相图，该相图在室温下支持中间反铁磁 (AFM) 螺旋自旋结构 (HSS) 状态，该状态位于两个铁磁 (FM) 相之间。沿三个晶轴进行磁测量，以建立 HSS 状态的温度和场依赖性模型。这些结果表明，AFM 状态是沿c轴传播的螺旋有序螺旋，磁矩在ab中旋转-飞机。在施加的磁场下，AFM 状态在高场进入完全场极化的 FM 状态之前表现出向锥形有序的超磁转变。即使在ab平面内，原子力显微镜状态下的锥形排序也是各向异性的，并且可能会在传输测量中产生贝里相位效应。通过电阻率测量证实了来自状态密度计算的金属电导率，并且通过各种磁跃迁没有观察到异常行为。
• The thermochemical behavior of some binary shape memory alloys by high temperature direct synthesis calorimetry
  作者：S.V. Meschel、J. Pavlu、P. Nash

  DOI：10.1016/j.jallcom.2011.01.152

  日期：2011.4

  The standard enthalpies of formation of some shape memory alloys have been measured by high temperature direct synthesis calorimetry at 1373 K. The following results (in kJ/mol of atoms) are reported: CoCr (-0.3 +/- 2.9); CuMn (-3.7 +/- 3.2); Cu3Sn (-10.4 +/- 3.1); Fe2Tb (-5.5 +/- 2.4); Fe2Dy (-1.6 +/- 2.9); Fe17Tb2 (-2.1 +/- 3.1); Fe17Dy2 (-5.3 +/- 1.7); FePd3 (-16.0 +/- 2.7); FePt (-23.0 +/- 1.9); FePt3 (-20.7 +/- 2.3); NiMn (-24.9 +/- 2.6); TiNi (-32.7 +/- 1.0); TiPd (-60.3 +/- 2.5). The results are compared with some earlier experimental values obtained by calorimetry and by EMF technique. They are also compared with predicted values on the basis of the semi empirical model of Miedema and co-workers and with ab initio calculations when available. We will also assess the available information regarding the structures of these alloys. (C) 2011 Elsevier B.V. All rights reserved.
• The isothermal section of the Nd–Fe–Ga ternary system at 773K
  作者：J.Q. Li、W.H. Zhang、Y.J. Yu、F.S. Liu、W.Q. Ao、J.L. Yan

  DOI：10.1016/j.jallcom.2009.07.154

  日期：2009.11

  The isothermal section of the Nd-Fe-Ga ternary system at 773 K was constructed using X-ray diffraction analysis. Ten binary compounds, Nd2Fe17, Nd5Fe17, Nd9Ga4, Nd5Ga3, NdGa, NdGa2, FeGa3, Fe3Ga4, alpha-Fe6Ga5 and alpha-Fe3Ga, and three ternary compounds, NdFe2Ga8, NdFe5Ga7 and Nd6Fe13Ga were existed in this isothermal section. The solid solutions Nd2Fe17.00-15.57Ga0-1.43 (Th2Zn17-type structure, space group R (3) over barm, NdFe5.46-4.65Ga6.(54-7.35) (ThMn12-type structure, space group 14/mmm) and Nd6Fe13.0-12.Ga-0(1.0-2.0) (La6Co11Ga3-type structure, space group 14/mcm) were formed by substitution of Ga for Fe in the compounds Nd2Fe17, NdFe5Ga7 and Nd6Fe13Ga at 773 K, respectively. The ternary compound NdFe2Ga8 is CaCo2Al8-type (space group Pbam) with a = 1.43742 (4), b = 1.24601 (4), c = 0.40479 (1)). The homogeneity range of NdGa2 is from 66.7 to 74.7 at.% Gain Nd-Ga side but the solid solubility of Fe in this compound is very small. The homogeneity ranges of Nd6Fe13Ga and NdFe5Ga7 are from 5.0 to 10.0 and from 50.3 to 56.5 at.% Ga, respectively. The maximum solid solubilities of Ga in Nd2Fe17 is 7.5. The homogeneity ranges for the other compounds are small. (C) 2009 Elsevier B.V. All rights reserved.