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Multilevel control of the metastable states in a manganite film

机译:锰薄膜中亚稳态的多级控制

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摘要

For high density memory applications, the dynamic switching between multilevel resistance states per cell is highly desirable, and for oxide-based memory devices, the multistate operation has been actively explored. We have previously shown that for La_(2/3)Ca_(1/3)MnO_3 films, the antiferromagnetic charge-ordered-insulator (COI) phase can be induced via the anisotropic epitaxial strain, and it competes with the doping-determined ferromagnetic-metal (FMM) ground state in a wide temperature range. Here, we show that for the phase competitions, in various magnetic fields and/or thermal cycling, the reappearance of the COI phase and thus the resistance and magnetization can be manipulated and quantified in a multilevel manner at lower temperatures. Furthermore, by using a high-field magnetic force microscope, we image the COI/FMM domain structures in accordance with the transport measurements, and find that the evolving domains or the phase fraction ratios do underline the metastability of the reappeared COI droplets, possibly protected by the energy barriers due to accommodation strain. These results may add new insights into the design and fabrication of future multilevel memory cells.
机译:对于高密度存储器应用,非常需要每个单元的多级电阻状态之间的动态切换,而对于基于氧化物的存储器件,已经积极探索了多状态操作。先前我们已经表明,对于La_(2/3)Ca_(1/3)MnO_3薄膜,可以通过各向异性外延应变感应出反铁磁电荷有序绝缘体(COI)相,并且它与掺杂确定的铁磁竞争-金属(FMM)在宽温度范围内处于基态。在这里,我们表明,对于相竞争,在各种磁场和/或热循环中,可以在较低温度下以多级方式操纵和量化COI相的出现,从而实现电阻和磁化强度的量化。此外,通过使用高场磁力显微镜,我们根据传输测量结果对COI / FMM畴结构进行了成像,发现不断发展的畴或相分数比率确实突出了重新出现的COI液滴的亚稳性,可能受到保护由于住宿压力而导致的能量障碍。这些结果可能为未来的多级存储单元的设计和制造增加新的见识。

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  • 来源
    《Journal of Applied Physics 》 |2017年第24期| 245304.1-245304.6| 共6页
  • 作者单位

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China;

    High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China,High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China,Collaborative Innovation Center of Advanced Microstructure, Nanjing 210093, China;

    Department of Physics and Hefei National Laboratory for Physical Sciences at Microscale,University of Science and Technology of China, Hefei 230026, China,High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China,Collaborative Innovation Center of Advanced Microstructure, Nanjing 210093, China;

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