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Magnetic structure and anisotropy of YFe_6Ga_6 and HoFe_6Ga_6

机译:YFe_6Ga_6和HoFe_6Ga_6的磁结构和各向异性

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The magnetic structure of RFe_6Ga_6 intermetallic compounds with R = Y, Ho have been determined by neutron powder diffraction, ~(57)Fe Mossbauer spectroscopy, AC susceptibility, TGA (Thermo-Gravimetric Analysis) and magnetization measurements. Both compounds crystallize in the tetragonal ThMn_(12) structure (space group 14/mmm) with the magnetic structure of YFe_6Ga_6 consisting of a simple ferromagnetic alignment of Fe moments in the basal plane with a Curie temperature of 475(5) K. Gallium atoms are found to fully occupy the 8i site, with Fe and Ga atoms equally distributed over the 8j site, whilst Fe atoms fully occupy the 8f site. The average Fe moments are 1.68(10) μ_B and 1.46(10) μ_B at 15 and 293 K, respectively. The average room temperature Fe magnetic moments determined by neutron diffraction are inoverall agreement with the average Fe moment deduced from Mossbauer spectroscopy and bulk magnetization measurements on this compound. The magnetic anisotropy of the compound HoFe_6Ga_6 is also planar in the temperature range 6-290 K, with Ho magnetic moments of 9.28(20) μ_B and 2.50(20) μ_B at 6 K and 290 K, respectively, coupled anti-ferromagnetically to the Fe sublattice and a Curie temperature of 460(10) K. The magneto-crystalline anisotropies of both compounds are comparable at low temperatures.
机译:通过中子粉末衍射,〜(57)Fe Mossbauer光谱,AC磁化率,TGA(热重分析)和磁化强度测量,确定Re = Y,Ho的RFe_6Ga_6金属间化合物的磁性结构。两种化合物均以四方ThMn_(12)结构(空间群14 / mmm)结晶,其YFe_6Ga_6磁性结构由基面上Fe矩的简单铁磁排列组成,居里温度为475(5)K。镓原子被发现完全占据了8i位,而Fe和Ga原子平均分布在8j位上,而Fe原子则完全占据了8f位。 15和293 K时的平均Fe矩分别为1.68(10)μ_B和1.46(10)μ_B。由中子衍射确定的平均室温Fe磁矩与由Mossbauer光谱法和对该化合物的体磁化测量得出的平均Fe矩总体上是一致的。化合物HoFe_6Ga_6的磁各向异性在6-290 K的温度范围内也是平面的,在6 K和290 K时的Ho磁矩分别为9.28(20)μ_B和2.50(20)μ_B,与铁磁耦合。铁的亚晶格和居里温度为460(10)K。这两种化合物的磁晶各向异性在低温下是可比的。

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