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首页> 外文期刊>Physical review >Glassy magnetic phase driven by short-range charge and magnetic ordering in nanocrystalline La_(1/3)Sr_(2/3)FeO_(3-δ): Magnetization, Mossbauer, and polarized neutron studies
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Glassy magnetic phase driven by short-range charge and magnetic ordering in nanocrystalline La_(1/3)Sr_(2/3)FeO_(3-δ): Magnetization, Mossbauer, and polarized neutron studies

机译:纳米晶La_(1/3)Sr_(2/3)FeO_(3-δ)中短程电荷和磁有序驱动的玻璃态磁相:磁化,莫斯鲍尔和极化中子研究

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摘要

The charge ordered La_(1/3)Sr_(2/3)FeO_(3-δ) (LSFO) in bulk and nanocrystalline forms are investigated using ac and dc magnetization, Mossbauer, and polarized neutron studies. A complex scenario of short-range charge and magnetic ordering is realized from the polarized 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 Mossbauer results. The refinement of magnetic diffraction peaks provides magnetic moments of Fe~(3+) and Fe~(5+) are about 3.15 μB and 1.57 μb for bulk, and 2.7 μ-b and 0.53 μb 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 ~70 nm, which is zero for the bulk counterpart. A strong frequency dependence of ac susceptibility reveals cluster-glass-like transition around ~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:电荷和有序La_(1/3)Sr_(2/3)FeO_(3-δ)(LSFO)的体积和纳米晶形式使用交流和直流磁化,Mossbauer和极化中子研究进行了研究。通过对纳米晶体样品中的极化中子研究,实现了短程电荷和磁有序性的复杂情况。与Mossbauer结果相比,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+)之间电荷歧化的任何改变。磁衍射峰的细化提供了Fe〜(3+)和Fe〜(5+)的磁矩分别为约3.15μB和1.57μb(对于大块),以及2.7μb和0.53μb(对于纳米晶体样品)。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。引人注目的是,在5 K时,EB场的平均尺寸约为70 nm,其值高达4.4 kOe,而对于大体积的EB场则为零。交流磁化率与频率的强相关性表明,在约65 K附近出现了簇状玻璃状转变,在此以下出现了EB。总体结果表明,有限尺寸效应指导了由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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  • 来源
    《Physical review》 |2012年第10期|p.104416.1-104416.9|共9页
  • 作者单位

    Department of Solid State Physics, Indian Association for the Cultivation of Science, Jadavpur, Kolkata 700032, India;

    Department of Solid State Physics, Indian Association for the Cultivation of Science, Jadavpur, Kolkata 700032, India,Department of Physics, Raghunathpur College, Raghunathpur, Purulia 723133, India;

    Department of Solid State Physics, Indian Association for the Cultivation of Science, Jadavpur, Kolkata 700032, India;

    Department of Solid State Physics, Indian Association for the Cultivation of Science, Jadavpur, Kolkata 700032, India;

    Department of Physics and CICECO, University ofAveiro, 3810-193, Aveiro, Portugal,Department of electronics & Communications, IT- GGV, Bilaspur 495009, India;

    Department of Physics and CICECO, University ofAveiro, 3810-193, Aveiro, Portugal;

    Departament de Fisica Fonamental and Institute of Nanoscience and Nanotechnology (IN2UB), Facultat de Fisica, Universitat de Barcelona, Av. Diagonal 647, 08028 Barcelona, Spain;

    JCNS, Forschungszentrum Juelich, Outstation at FRMII, Lichtenbergstrasse 1, 85747 Garching, Germany;

    Science Division, Institut Laue-Langevin BP 156, 38042 Grenoble Cedex 9, France;

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  • 正文语种 eng
  • 中图分类
  • 关键词

    fine-particle systems; nanocrystalline materials;

    机译:细颗粒系统;纳米晶材料;

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