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η-碳化硼型氮化物(Ni,Co,Fe)2(Ga,Ge)Mo3N 的磁有序。

Magnetic ordering in nitrides with the eta-carbide structure, (Ni,Co,Fe)2(Ga,Ge)Mo3N.

机构信息

Inorganic Chemistry Laboratory, University of Oxford, South Parks Road, Oxford, OX1 3QR, United Kingdom.

出版信息

Inorg Chem. 2010 Feb 1;49(3):1133-43. doi: 10.1021/ic902069w.

DOI:10.1021/ic902069w
PMID:20030337
Abstract

Compositions in the series Ni(2-x)Co(x)GeMo(3)N (0 < or = x < or = 2), Co(2)Ge(1-x)Ga(x)Mo(3)N (0 < x < or = 0.7), Co(2-x)Fe(x)GeMo(3)N (0 < or = x < or = 2), and Co(2-x)Fe(x)Ge(0.5)Ga(0.5)Mo(3)N (0 < or = x < or = 0.8) have been synthesized by the reductive nitridation of binary oxides and studied by appropriate combinations of magnetometry, transport measurements, neutron diffraction, and Mossbauer spectroscopy. All of these compositions adopt the cubic eta-carbide structure (a approximately 11.11 A) and show a resistivity of approximately 10(-3) Omega cm. No long-range magnetic order was observed in Ni(2-x)Co(x)GeMo(3)N, although evidence of spin freezing was observed in Co(2)GeMo(3)N. The introduction of gallium into this composition leads to the onset of antiferromagnetic ordering at 90 K in Co(2)Ge(0.3)Ga(0.7)Mo(3)N. The magnetic structure consists of an antiferromagnetic arrangement of ferromagnetic Co(4) groups, with an ordered magnetic moment of 0.48(9) micro(B) per cobalt atom. The same magnetic structure is found in Co(0.5)Fe(1.5)GeMo(3)N and Co(1.2)Fe(0.8)Ge(0.5)Ga(0.5)Mo(3)N. The former orders above room temperature with an average moment of 1.08(3) mu(B) per transition-metal site, and the latter at 228 K with an average moment of 1.17(4) micro(B) per site. The magnetic behavior of these compounds is discussed in terms of the electron count within each series.

摘要

Ni(2-x)Co(x)GeMo(3)N(0 <= x <= 2)、Co(2)Ge(1-x)Ga(x)Mo(3)N(0 < x <= 0.7)、Co(2-x)Fe(x)GeMo(3)N(0 <= x <= 2)和 Co(2-x)Fe(x)Ge(0.5)Ga(0.5)Mo(3)N(0 <= x <= 0.8)系列的组成物通过二元氧化物的还原氮化合成,并通过磁强计、输运测量、中子衍射和穆斯堡尔光谱学的适当组合进行研究。所有这些组成物都采用立方 eta-碳化物结构(a 约为 11.11 A),电阻率约为 10(-3) Omega cm。尽管在 Co(2)GeMo(3)N 中观察到自旋冻结的证据,但在 Ni(2-x)Co(x)GeMo(3)N 中未观察到长程磁有序。在该组成物中引入镓会导致 Co(2)Ge(0.3)Ga(0.7)Mo(3)N 中在 90 K 时出现反铁磁有序。磁结构由铁磁 Co(4)基团的反铁磁排列组成,每个钴原子的有序磁矩为 0.48(9) micro(B)。在 Co(0.5)Fe(1.5)GeMo(3)N 和 Co(1.2)Fe(0.8)Ge(0.5)Ga(0.5)Mo(3)N 中也发现了相同的磁结构。前者在室温以上有序,每个过渡金属位的平均磁矩为 1.08(3) mu(B),后者在 228 K 时有序,每个位的平均磁矩为 1.17(4) micro(B)。这些化合物的磁行为根据每个系列中的电子计数进行讨论。

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