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Disorder-Driven Spin-Reorientation in Multiferroic $h-YMn_{1-x}Fe_xO_3$

机译:multiferroic $ h-Ymn_ {1-x} Fe_xO_3 $中的无序驱动自旋重定向

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摘要

Magnetic structure evolution of multiferroic hexagonal $YMn_{1-x}Fe_{x}O_{3}$(${x} = 0, 0.05,$ and $0.1$) has been studied by carrying out detailedtemperature-dependent neutron diffraction at zero- and 5T-fields. Thermodynamicdata confirm antiferromagnetic ordering at $T_{N}$ in all the compositions. Oursub-$T_{N}$ neutron diffraction results assign the magnetic structure of pure$YMnO_3$ to $\Gamma_{1}$ irreducible representation. Over theperturbative-doping range, the magnetic configuration changes via$\Gamma_{1}+\Gamma_{2}$ for $YMn_{0.95}Fe_{0.05}O_{3}$ on to $\Gamma_{2}$ for$YMn_{0.9}Fe_{0.1}O_{3}$, as the maiden compositional analogue ofspin-reorientation; its occurrence in temperature-domain already reported forseveral manganites. Moreover, while the large thermal isostructural changesobserved above ${T}_{N}$ are subdued in the ordered state, small alterations bythe applied 5T-field are relatively uniform across, confirming strongmagneto-elastic nature of the system. Decrease of the ordered magnetic moment($\mu_{ord}$) and planar magnetic frustration noted with Fe-doping is enhancedby the applied field, apparently through canting.
机译:通过在零温度下进行与温度有关的中子衍射研究,研究了多铁六角形$ YMn_ {1-x} Fe_ {x} O_ {3} $($ {x} = 0、0.05,$和$ 0.1 $)的磁性结构演化-和5T战场。热力学数据证实在所有成分中反铁磁有序为$ T_ {N} $。我们的sub- $ T_ {N} $中子衍射结果将纯$ YMnO_3 $的磁性结构赋予$ \ Gamma_ {1} $不可约表示。在微扰掺杂范围内,磁配置通过$ YMn_ {0.95} Fe_ {0.05} O_ {3} $的$ \ Gamma_ {1} + \ Gamma_ {2} $变为$$ Gamma_ {2} $ YMn_ {0.9} Fe_ {0.1} O_ {3} $,作为自旋取向的首个组成类似物;其在温度范围内的存在已经报道了几种锰矿。此外,虽然在有序状态下可以观察到在$ {T} _ {N} $以上观察到的较大的热等结构变化,但所施加的5T场的较小变化在整个过程中是相对均匀的,从而确认了系统的强磁弹性性质。显然,通过倾斜,施加的磁场增强了有序磁矩($ \ mu_ {ord} $)的减小和铁掺杂引起的平面磁挫折。

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