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Glassy magnetic phase driven by short-range charge and magnetic ordering in nanocrystalline La1/3Sr2/3FeO3−δ: Magnetization, Mössbauer, and polarized neutron studies

机译:纳米晶La1 / 3Sr2 /3FeO3-δ中短程电荷和磁有序驱动的玻璃态磁相:磁化,Mössbauer和极化中子研究

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摘要

The charge ordered La$_{1/3}$Sr$_{2/3}$FeO$_{3-delta}$ (LSFO) in bulk and nanocrystalline forms are investigated using ac and dc magnetization, M'{o}ssbauer, and polarised neutron studies. A complex scenario of short range charge and magnetic ordering is realized from the polarised neutron studies in nanocrystalline specimen. This short range ordering does not involve any change in spin state and modification in the charge disproportion between Fe$^{3+}$ and Fe$^{5+}$ compared to bulk counterpart as evident in the M'{o}ssbauer results. The refinement of magnetic diffraction peaks provides magnetic moments of Fe$^{3+}$ and Fe$^{5+}$ are about 3.15$mu_B$ and 1.57$mu_B$ for bulk, and 2.7$mu_B$ and 0.53$mu_B$ for nanocrystalline specimen, respectively. The destabilization of charge ordering leads to magnetic phase separation, giving rise to the robust exchange bias (EB) effect. Strikingly, EB field at 5 K attains a value as high as 4.4 kOe for average size $sim$ 70 nm, which is zero for the bulk counterpart. A strong frequency dependence of ac susceptibility reveals cluster-glass like transition around $sim$ 65 K, below which EB appears. Overall results propose that finite size effect directs the complex glassy magnetic behavior driven by unconventional short range charge and magnetic ordering, and magnetic phase separation appears in nanocrystalline LSFO.
机译:使用交流和直流磁化强度M'{o来研究散装和纳米晶形式的有序La $ _ {1/3} $ Sr $ _ {2/3} $ FeO $ _ {3-delta} $(LSFO) } ssbauer和极化中子研究。纳米晶体样品中的极化中子研究实现了短距离电荷和磁有序的复杂情况。与M'{o} ssbauer所证明的相比,这种短程有序不涉及自旋态的任何变化,也没有涉及Fe $ ^ {3 +} $和Fe $ ^ {5 +} $之间的电荷不平衡的改变。结果。磁衍射峰的细化提供了Fe $ ^ {3 +} $和Fe $ ^ {5 +} $的磁矩,分别约为3.15 $ mu_B $和1.57 $ mu_B $,以及2.7 $ mu_B $和0.53 $ mu_B $分别代表纳米晶体标本。电荷排序的不稳定导致磁相分离,从而产生稳健的交换偏压(EB)效应。令人惊讶的是,在5 K时,EB场的平均尺寸为sim $ 70 nm,其值高达4.4 kOe,对于大体积对应物为零。交流磁化率与频率的强烈相关性表明,类似簇状玻璃的转变在$ sim $ 65 K附近,在其下方出现EB。总体结果表明,有限尺寸效应指导了非常规短程电荷和磁有序驱动的复杂玻璃态磁行为,并且纳米晶LSFO中出现了磁相分离。

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