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Magnetic order of intermetallic FeGa$_{3-y}$Ge$_y$ studied by $\mu$SR and $^{57}$Fe M'ossbauer spectroscopy

机译:金属间化合物的磁性顺序$ _ {3-y} $ Ge $ _y $由$ \ mu $ sR研究   和$ ^ {57} $ Fe m \“ossbauer光谱学

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摘要

Temperature dependent magnetization, muon spin rotation and $^{57}$FeM\"ossbauer spectroscopy experiments performed on crystals of intermetallicFeGa$_{3-y}$Ge$_{y}$ ($y=0.11,0.14,0.17,0.22,0.27$, $0.29,0.32$) are reported.Whereas at $y=0.11$ even a sensitive magnetic microprobe such as $\mu$SR doesnot detect magnetism, all other samples display weak ferromagnetism with amagnetic moment of up to 0.22 $\mu_B$ per Fe atom. As a function of doping andof temperature a crossover from short range to long range magnetic order isobserved, characterized by a broadly distributed spontaneous internal field.However, the $y=0.14$ and $y=0.17$ remain in the short range ordered state downto the lowest investigated temperature. The transition from short range to longrange order appears to be accompanied by a change of the character of the spinfluctuations, which exhibit spin wave excitations signature in the LRO part ofthe phase diagram. M\"ossbauer spectroscopy for $y=0.27$ and 0.32 indicatesthat the internal field lies in the plane perpendicular to the crystallographic$c$ axis. The field distribution and its evolution with doping suggest that thedetails of the Fe magnetic moment formation and the consequent magnetic stateare determined not only by the dopant concentration but also by the way thereplacement of the Ga atoms surrounding the Fe is accomplished.
机译:对金属间化合物FeGa $ _ {3-y} $ Ge $ _ {y} $的晶体进行的温度依赖性磁化强度,μ自旋旋转和$ ^ {57} $ FeM \“ ossbauer光谱实验($ y = 0.11,0.14,0.17,报告为0.22,0.27 $,0.29、0.32 $),而在$ y = 0.11 $处,即使像$ \ mu $ SR这样的灵敏磁性微探针也不能检测到磁性,而其他所有样品都显示弱的铁磁性,其磁矩高达0.22 $。每个Fe原子的μmuB$,作为掺杂和温度的函数,观察到了从短程到长程磁阶的交叉,其特征是自发的内部磁场分布广泛,但是,仍保持$ y = 0.14 $和$ y = 0.17 $。在短程有序状态下降到最低研究温度,从短程到长程的转变似乎伴随着自旋涨落特性的变化,在相图的LRO部分显示出自旋波激发特征。 “ $ y = 0.27 $和0.32的ossbauer光谱表明内部场位于垂直于晶体学$ c $轴的平面上。场分布及其随掺杂的演变表明,Fe磁矩形成的细节和随之产生的磁态不仅取决于掺杂剂的浓度,而且取决于完成包围Fe的Ga原子的位置。

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