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Thickness dependence of exchange coupling in (111)-oriented perovskite oxide superlattices

机译:(111)取向钙钛矿氧化物超晶格中交换耦合的厚度依赖性

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摘要

Epitaxial La_(0.7)Sr_(0.3)MnO_3 (LSMO)/La_(0.7)Sr_(0.3)FeO_3 (LSFO) superlattices on (111)-oriented SrTiO_3 substrates with sublayer thicknesses ranging from 3 to 60 unit cells (u.c.) were synthesized and characterized. Detailed analysis of their structural, electronic, and magnetic properties were performed to explore the effect of sublayer thickness on the magnetic structure and exchange coupling at (11 l)-oriented perovskite oxide interfaces. In the ultrathin limit (3-6 u.c), we find that the antiferromagnetic (AF) properties of the LSFO sublayers are preserved with an out-of-plane canting of the AF spin axis, while the ferromagnetic (FM) properties of the LSMO sublayers are significantly depressed. For thicker LSFO layers (>9 u.c), the out-of-plane canting of the AF spin axis is only present in superlattices with thick LSMO sublayers. As a result, exchange coupling in the form of spin-flop coupling exists only in superlattices which display both robust ferromagnetism and out-of-plane canting of the AF spin axis.
机译:合成了(111)取向SrTiO_3衬底上亚层厚度为3至60个晶胞(uc)的外延La_(0.7)Sr_(0.3)MnO_3(LSMO)/ La_(0.7)Sr_(0.3)FeO_3(LSFO)超晶格和特点。对其结构,电子和磁性进行了详细分析,以探索亚层厚度对磁性结构和在(11 l)取向钙钛矿氧化物界面处的交换耦合的影响。在超薄极限(3-6 uc)中,我们发现LSFO子层的反铁磁(AF)特性通过AF自旋轴的平面外倾斜得以保留,而LSMO的铁磁(FM)特性子层明显凹陷。对于较厚的LSFO层(> 9 u.c),仅在具有较厚LSMO子层的超晶格中才会出现AF自旋轴的面外倾斜。结果,自旋触发器耦合形式的交换耦合仅存在于超晶格中,该超晶格同时显示出强大的铁磁性和AF自旋轴的平面外倾斜。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2016年第10期|104403.1-104403.9|共9页
  • 作者单位

    Department of Chemical Engineering and Materials Science, University of California, Davis, Davis, California 95616, USA;

    Department of Chemical Engineering and Materials Science, University of California, Davis, Davis, California 95616, USA;

    Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA;

    Center for Nanophase Materials Science, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Center for Nanophase Materials Science, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    Department of Chemical Engineering and Materials Science, University of California, Davis, Davis, California 95616, USA;

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