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Anisotropic magnetic and transport properties of UNiGe

机译:UNiGe的各向异性磁和输运性质

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摘要

Magnetism in UNiGe which adopts the orthorhombic TiNiSi type of structure with lattice constants a=700.7 pm, b =423.7 pm, c=720.7 pm is strongly anisotropic. The Curie-Weiss behaviour of the susceptibility above 80 K yields values of /spl Thetasub p/ equal to -98, 3 and 41 K for the a, b and c axis, respectively. Also the electrical resistivity is anisotropic and reflects magnetic phase transitions at 41.5 and 50 K, in very good agreement with specific-heat data. An antiferromagnetic structure of U moments of about 1.4 /spl musub B/ with a propagation vector q=(0, 0.5, 0.5) can be concluded from neutron-diffraction studies at low temperatures. Two metamagnetic transitions are observed in high-field magnetization data at 4.2 K in fields applied along the b (at 17 and 25 T) and c (at 3 and 10 T) axes yielding parallel alignment of the magnetic moments in fields above the second transition. The magnetization measured at 35 T amounts to 1.45 /spl musub Bf.u. The huge magnetic anisotropy is reflected in the weak linear magnetic response to fields along the a axis yielding only 0.23 /spl musub Bf.u. at 35 T. The destruction of antiferromagnetic ordering in high fields is accompanied by a reduction of about 80 of the electrical resistivity. The huge magnetic anisotropy and giant magnetoresistance which is also observed in other UTX compounds (T=transition metal, X=p-metal) can be understood in terms of anisotropic 5f-ligand hybridization.
机译:UNiGe中采用正交各向异性TiNiSi型结构且晶格常数a = 700.7 pm,b = 423.7 pm,c = 720.7 pm的磁性是强各向异性的。高于80 K的磁化率的居里-魏斯行为产生的/ spl Thetasub p /值分别等于a,b和c轴的-98、3和41K。而且,电阻率是各向异性的,并且反映了在41.5和50 K时的磁相变,与比热数据非常吻合。可以从低温下的中子衍射研究得出结论,U矩的反铁磁结构约为1.4 / spl musub B /,传播矢量为q =(0,0.5,0.5)。在沿b(17和25 T)和c(3和10 T)轴施加的磁场中,在4.2 K的高磁场磁化数据中观察到两个亚磁跃迁,产生了第二跃迁以上磁场中磁矩的平行排列。在35 T下测得的磁化强度为1.45 / spl musubBf.u。巨大的磁各向异性反映在对沿a轴的磁场的弱线性磁响应中,仅产生0.23 / spl musubBf.u。在35 T时。高磁场中反铁磁序的破坏伴随着电阻率的降低约80。可以从各向异性5f-配体杂交的角度理解在其他UTX化合物(T =过渡金属,X = p-金属)中也观察到的巨大的磁各向异性和巨大的磁阻。

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