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~(17)O NMR study of the doped electrons in lightly oxygen-deficient cubic SrMnO_(3-x)

机译:轻度缺氧的立方SrMnO_(3-x)中掺杂电子的〜(17)O NMR研究

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摘要

The spin susceptibility of the localized Mn(t_(2g)) electrons, χ_s, and the spatially distributed spin density of the doped electrons were investigated by ~(17)O nuclear magnetic resonance (NMR) in the paramagnetic (PM) and antiferromagnetic (AF) phases of electron-doped SrMnO_(3-x) ceramics with the cubic structure. Three lightly doped samples (2x < 0.015) were studied with T_N = 220 K-240 K. In the PM state χ_s increases gradually from T_N and reaches a broad maximum above ~ 1.5 T_N. The gapped behavior of χ_s indicates a low-dimensional short-range spin order persisting above T_N These short-range one-dimensional correlations are consistent with ~(17)O NMR results obtained at room temperature, which show that Mn magnetic moments are aligned along the edges of the cubic unit cell. Above 350 K all doped electrons are fast-moving e_g electrons. They provide the uniform polarization of the localized spins which increases χ_s and the increasing doping shifts the oxygen-deficient SrMnO_(3-x) oxide towards a ferromagnetic (FM) metallic state. At lower T the doped electrons are heterogeneously distributed in the oxide: The fraction of the fast-moving electrons diminishes and vanishes below 100 K, while the remaining doped electrons slow down their hopping and each of them creates a FM domain. These FM domains which are detected below 10 K by ~(55)Mn NMR can be considered as small-size magnetic polarons. Their T-activated hopping in the G-type AF lattice was probed by ~(17)O spin-echo experiments. The energy barrier of hopping shows a trend to grow with increasing doping, indicating that the de Gennes metallic ground state cannot be achieved in oxygen-deficient SrMnO_(3-x) oxides, probably due to detrimental oxygen vacancy defects.
机译:通过〜(17)O核磁共振(NMR)在顺磁(PM)和反铁磁(PM)中研究了局部Mn(t_(2g))电子的自旋磁化率χ_s,以及掺杂电子的空间分布自旋密度。 AF)具有立方结构的电子掺杂SrMnO_(3-x)陶瓷相。研究了三个轻度掺杂样品(2x <0.015),T_N = 220 K-240K。在PM状态下,χ_s从T_N逐渐增加,并在〜1.5 T_N以上达到最大。 χ_s的带隙行为表明低维短程自旋顺序在T_N之上持续存在。这些短程一维相关性与室温下获得的〜(17)O NMR结果一致,表明Mn磁矩沿立方晶胞的边缘。在350 K以上,所有掺杂电子都是快速移动的e_g电子。它们提供了局部自旋的均匀极化,从而使χ_s增大,并且掺杂的增加使缺氧的SrMnO_(3-x)氧化物向铁磁(FM)金属态移动。在较低的T下,掺杂的电子异质分布在氧化物中:在100 K以下,快速移动的电子的比例减小并消失,而其余的掺杂的电子则减慢其跃变,并且每个电子都产生FM域。通过〜(55)Mn NMR在10 K以下检测到的这些FM域可以看作是小型磁极化子。通过〜(17)O自旋回波实验探究了它们在G型AF晶格中的T激活跳跃。跳跃的能垒显示出随着掺杂增加而增长的趋势,表明可能由于有害的氧空位缺陷,在缺氧的SrMnO_(3-x)氧化物中无法达到de Gennes金属基态。

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  • 来源
    《Physical review》 |2016年第17期|174413.1-174413.10|共10页
  • 作者单位

    LPEM, ESPCI Paris, PSL Research University, CNRS, Sorbonne Universites, UPMC University, 10 rue Vauquelin, F-75005 Paris, France;

    LPEM, ESPCI Paris, PSL Research University, CNRS, Sorbonne Universites, UPMC University, 10 rue Vauquelin, F-75005 Paris, France,Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 620990 Ekaterinburg, Russia;

    Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 620990 Ekaterinburg, Russia;

    LPEM, ESPCI Paris, PSL Research University, CNRS, Sorbonne Universites, UPMC University, 10 rue Vauquelin, F-75005 Paris, France,Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 620990 Ekaterinburg, Russia;

    Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 620990 Ekaterinburg, Russia;

    Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 620990 Ekaterinburg, Russia;

    Russian Research Centre Kurchatov Institute, 123182 Moscow, Russia;

    Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 620990 Ekaterinburg, Russia;

    Department of Physics, Northern Illinois University, DeKalb, Illinois 60115, USA;

    Institute of Solid State Chemistry, Ural Branch of Russian Academy of Sciences, 620018 Ekaterinburg, Russia;

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