研究了镁合金在43% ~ 50% at的范围内。%Sb,揭示了MN2SB相的意外存在

Iwamoto Gy
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引用次数: 1

摘要

1898年Heusler1报道了有色金属磁性合金的发现,从那时起,这些合金在工业和科学装置上的研究和应用不断发展。Guillaud2描述了MnSb合金的可变居里温度(在90°C和314°C之间),完全通过化学计量学的变化(从45%到49%的Sb原子百分比(at.%Sb))来获得。至少有6种不同的相图被发表,除了发现时间较长外,它们仍然存在与MnSb相的最小/最大化学计量及其各自的Tc相关的一些不确定区域。Okamoto的相图3定义了该区域在室温至314℃范围内为45%和49%原子Sb,各自的Tc在90℃至314℃范围内变化。来自ICSD4的晶体学文件提供了相描述为Mn1.092Sb或Mn1.1Sb的参考。8个样本,从43%到50%不等。合成了Sb,覆盖了Mn1.092Sb相的全部范围。Guillaud 2报道了在90°C到314°C之间的可调磁转变,Teramoto和Van Run5证实了在400°C到700°C之间的退火温度与49% Sb原子的不相关,并绘制了部分相图(图1),其中MnSb稳定相随400°C时Sb的46到50%的温度变化,而在840°C时原子Sb的41% (%at.Sb)的单点描述了非线性行为。Teramoto和Van Run5报道,在400°C到700°C之间淬火不改变Tc,与退火或淬火温度无关,而仅与化学计量有关。Okamoto3报告了840°C时的包晶转变和可变Tc相关的化学计量从44%到49%。在400°C。Chen6确定了843℃时的包晶温度,400℃时Sb原子的化学量在45% ~ 49.5%之间,Vanyarkho7确定了841℃时的包晶温度,400℃时MnSb相的化学量在45% ~ 49%之间,Williams8报道了853℃时的包晶温度,573℃下的可变磁性范围在40% ~ 50%之间;和Kainzbauer9报道了830°C的包晶温度,MnSb相的Sb含量从45.5%到50.5at%不等。Guillaud2将MnSb合金中的反应描述为SOMT(二阶磁转变),而Nwodo10则报道了m2sb的自旋取向随Sn (Mn2Sb0.9Sn0.1)的下降而发生的fmt(一级磁转变),AFM-FI(反铁磁→铁磁)反应。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Study of MnSb alloy on the range of 43% to 50% of at.%Sb, revealed an unexpected presence of MN2SB phase
The discovery of nonferrous magnetic alloys was reported by Heusler1 in 1898 and since then the investigation and application of these alloys on industrial and scientific devices have been growing continuously. Guillaud2 described a variable Curie Temperature (between 90°C and 314°C) for MnSb alloy, obtained exclusively through the variation of the stoichiometry (from 45% to 49% in atomic percentage of Sb (at.%Sb). At least six different phase diagrams were published, besides the long time from its discovery, they still have some uncertain regions related to minimum/maximum stoichiometry of MnSb phase and its respective Tc. Okamoto’s phase diagram3 defines this region being from 45% and 49% atomic Sb at room temperature up to 314°C, and respective Tc varying from 90°C to 314°C. Crystallographic files from ICSD4 provide references where the phase is described as Mn1.092Sb or Mn1.1Sb. Eight samples, from 43% to 50% at. Sb was produced, covering the complete range of Mn1.092Sb phase. Guillaud 2 reported a tunable magnetic transition through stoichiometry between 90°C to 314°C, Teramoto & Van Run5 confirmed the non dependency of annealing temperature between 400°C and 700°C for 49% atomic of Sb, and plotted a partial phase diagram (Figure 1), where MnSb stable phase varies with temperature from 46 to 50%at of Sb at 400°C, and a single point at 41% atomic Sb (%at.Sb) at 840°C describing a non linear behavior. Teramoto & Van Run5 reported quenching from temperatures between 400°C to 700°C didn’t change the Tc, being independent of annealing or quenching temperature, but only related to stoichiometry. Okamoto3 reported a peritectic transition at 840°C and variable Tc related stoichiometry from 44% to 49% at.Sb. at 400°C. Chen6 identified the peritectic temperature at 843°C and the stoichiometry between 45% and 49.5% atomic of Sb at 400°C, Vanyarkho7 r e p o r t e d the peritectic temperature at 841°C and the MnSb phase from 45% to 49% at 400°C, Williams8 reported the peritectic temperature at 853°C and variable magnetic range from 40% to 50% below 573; and Kainzbauer9 reported the peritectic temperature at 830°C and limits of MnSb phase from 45.5% to 50.5at% of Sb. Although Guillaud2 described the reaction at MnSb alloy as a SOMT (Second Order Magnetic Transition), Nwodo10 reported a FOMT (first order magnetic transition), AFM-FI (Antiferromagnetic→Ferrimagnetic) reaction, attributed to a spin reorientation of Mn2Sb dropped with Sn (Mn2Sb0.9Sn0.1).
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