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Enhancement of A′-site Mn~(3+) spin ordering by B-site Mn~(4+) substitution in quadruple perovskite PbMn_3Cr_3MnO_(12)

机译:通过B-PAITE MN〜(4+)旋转排序在四肢钙钛矿PBMN_3CR_3MNO_(12)中的B-PAITE MN〜(3+)旋转排序的增强

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摘要

An A-site ordered but B-site disordered quadruple perovskite oxide PbMn_3Cr_3MnO_(12) was synthesized by high-pressure and high-temperature methods. The compound crystallizes in space group Im-3 with the charge distribution of Pb~(2+)Mn~(3+)_3Cr~(3+)_3Mn~(4+)O_(12). Three antiferromagnetic phase transitions are found to occur at T_(N1)≈ 155, T_(N2)≈ 81, and T_(N3)≈ 74 K, respectively, due to the complex B-site and A'-B intersite spin interactions. Compared with the isostructural LaMn_3Cr_4O_(12) with negligible A'-B intersite spin coupling, the substitution of Mn~(4+), which has identical electronic configuration to that of Cr~(3+) (t_(2g)~3), into the B site can introduce A'-B intersite spin interactions. As a result, the A'-site spin-related ordering temperature increases significantly, while the B-site one remains little changed in the current PbMn_3Cr_3MnO_(12). This work opens up a way to enhance the A'-site spin ordering temperature in quadruple perovskite oxides.
机译:通过高压和高温方法合成了一个有序但是有序的但B-位点紊乱的四重钙钛矿PBMN_3CR_3MNO_(12)。 该化合物在空间组IM-3中结晶,具有Pb〜(2+)Mn〜(3 +)_ 3Cr〜(3 +)_ 3Mn〜(4 +)O_(12)的电荷分布。 发现,由于复合B位点和A'-B间隙旋转相互作用,发现在T_(n1)≈15,t_(n2)≈81和t_(n3)≈7k中发生三种反铁磁相转变。 与IsoStrontuctuctureLAMN_3CR_4O_(12)相比,具有可忽略的A'-B间隙旋转耦合,替代Mn〜(4+),其具有与Cr〜(3+)(T_(2g)〜3)相同的电子配置 ,进入B网站可以介绍A'-B间隙自旋相互作用。 结果,A'-现场的自旋相关的订购温度显着增加,而B-Site一个在当前PBMN_3CR_3MNO_(12)中仍然很小。 这项工作开辟了一种方法来增强四重钙钛矿氧化物中A'-位点的旋转排序温度。

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  • 来源
    《Applied Physics Letters》 |2021年第26期|262403.1-262403.5|共5页
  • 作者单位

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China;

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China Songshan Lake Materials Laboratory Dongguan Guangdong 523808 China;

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Max Planck Institute for Chemical Physics of Solids Dresden 01187 Germany;

    Department of Physics National Chung Cheng University Chiayi 62102 Taiwan;

    National Synchrotron Radiation Research Center 101 Hsin-Ann Road Hsinchu 30076 Taiwan;

    National Synchrotron Radiation Research Center 101 Hsin-Ann Road Hsinchu 30076 Taiwan;

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China Songshan Lake Materials Laboratory Dongguan Guangdong 523808 China;

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