Chinese Physics B, Volume. 29, Issue 9, (2020)

Tuning magnetic anisotropy by interfacial engineering in La2/3Sr1/3Co1 – xMnxO2.5 + δ/La2/3Sr1/3MnO3/La2/3Sr1/3Co1 – xMnxO2.5 + δtrilayers

Hai-Lin Huang1,2, Liang Zhu1,2, Hui Zhang1,2, Jin-E Zhang1,2, Fu-Rong Han1,2, Jing-Hua Song1,2, Xiaobing Chen1,2, Yuan-Sha Chen1,2, Jian-Wang Cai1,2, Xue-Dong Bai1,2, Feng-Xia Hu1,2, Bao-Gen Shen1,2,3, and J-Rong Sun1,2,3、†
Author Affiliations
  • 1Beijing National Laboratory for Condensed Matter Physics & Institute of Physics, Chinese Academy of Sciences, Beijing 0090, China
  • 2School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Songshan Lake Materials Laboratory, Dongguan 52808, China
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    Figures & Tables(5)
    (a) The sketch diagram of LSCMO/LSMO/LSCMO (x = 0–0.7) trilayers. (b) The surface morphology of the LSCO/LSMO/LSCO trilayer; the scale of the image is 5 × 5 μm2. (c) The x-ray diffraction patterns of LSCMO/LSMO/LSCMO trilayers. The multi-peaks indicate the high crystal quality of the trilayers. The reciprocal space mappings of the (1¯03) reflections of (d) LSCO/LSMO/LSCO and (e) LSCMO/LSMO/LSCMO (x = 0.7) trilayers.
    Typical high-angle annular dark-field image of the cross-section of the LSCMO/LSMO/LSCMO trilayers with (a) x = 0, (b) x = 0.3, and (c) x = 0.7, respectively, recorded along the [100] zone. Red dashed-line marks the LSCMO/LSMO interface and the yellow arrows represent the dark stripes.
    Thermomagnetic curves of the (a) LSCO/LSMO/LSCO and (b) LSCMO/LSMO/LSCMO (x = 0.7) trilayers. The data were acquired in field-cooling mode with in-plane or out-of-plane applied fields. Blue and orange areas highlight the difference of the magnetic moments along two measuring directions. The moment as a function of applied fields for the (c) LSCO/LSMO/LSCO and (d) LSCMO/LSMO/LSCMO (x = 0.7) trilayers, extracted from the thermomagnetic data at T = 10 K. The shaded area corresponds to the energy required to orientate the magnetic moment of trilayer from the hard axis to the easy axis.
    (a) Thermomagnetic curves of the LSCMO/LSMO/LSCMO (x = 0–0.7) trilayers along the in-plane and out-of plane directions under an applied field of 0.05 T. (b) The KA as a function of temperature for the LSCMO/LSMO/LSCMO (x = 0–0.7) trilayers. Here, the positive value of KA indicates the perpendicular magnetic anisotropy. (c) The KA as a function of Mn concentration for the LSCMO/LSMO/LSCMO (x = 0–0.7) trilayers at 10 K. The blue curve and light green curve are the results extracted from thermomagnetic curves and hysteresis curves, respectively.
    Normalized Mn-XAS spectra for the (a) [LSCO(4 uc)/LSMO(4 uc)]5 and (b) [LSCMO(4 uc)/LSMO(4 uc)]5 (x = 0.7) multilayers, measured with the optical polarization parallel (E||a, IIP) or perpendicular (E||c, IOP) to the film plane. The sketch shows the experimental setup. Bottom panels are the corresponding XLD spectra and the shaded areas provide the information on orbital occupancy. The arrow marks the spin orientation of the LSMO layer.
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    Hai-Lin Huang, Liang Zhu, Hui Zhang, Jin-E Zhang, Fu-Rong Han, Jing-Hua Song, Xiaobing Chen, Yuan-Sha Chen, Jian-Wang Cai, Xue-Dong Bai, Feng-Xia Hu, Bao-Gen Shen, J-Rong Sun. Tuning magnetic anisotropy by interfacial engineering in La2/3Sr1/3Co1 – xMnxO2.5 + δ/La2/3Sr1/3MnO3/La2/3Sr1/3Co1 – xMnxO2.5 + δtrilayers[J]. Chinese Physics B, 2020, 29(9):

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    Paper Information

    Received: Jun. 4, 2020

    Accepted: --

    Published Online: Apr. 29, 2021

    The Author Email: Sun J-Rong (jrsun@iphy.ac.cn)

    DOI:10.1088/1674-1056/aba2e2

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