• Chinese Physics B
  • Vol. 29, Issue 9, (2020)
Xin Wen1, Rui Wu1、†, Wen-Yun Yang1、2、3, Chang-Sheng Wang1、2、3, Shun-Quan Liu1、2、3, Jing-Zhi Han1、2、3, and Jin-Bo Yang1、2、3
Author Affiliations
  • 1State Key Laboratory for Mesoscopic Physics and School of Physics, Peking University, Beijing 0087, China
  • 2Beijing Key Laboratory for Magnetoelectric Materials and Devices, Beijing 100871, China
  • 3Collaborative Innovation Center of Quantum Matter, Beijing 100871, China
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    DOI: 10.1088/1674-1056/aba611 Cite this Article
    Xin Wen, Rui Wu, Wen-Yun Yang, Chang-Sheng Wang, Shun-Quan Liu, Jing-Zhi Han, Jin-Bo Yang. Room-temperature electric control of exchange bias effect in CoO1 – δ/Co films using Pb(Mg1/3Nb2/3)0.7Ti0.3O3 (110) substrates[J]. Chinese Physics B, 2020, 29(9): Copy Citation Text show less
    (a) Schematic of Cu/CoO1–δ/Co/Cu stack grown on PMN-PT(110) substrate and the configuration used for applying an electric field. (b) Cross-sectional TEM image of the stack.
    Fig. 1. (a) Schematic of Cu/CoO1–δ/Co/Cu stack grown on PMN-PT(110) substrate and the configuration used for applying an electric field. (b) Cross-sectional TEM image of the stack.
    (a) The ZFC magnetic hysteresis loops measured with magnetic fields applied along the [1 – 10] and [001] directions. (b) A schematic of the strain induced in the PMN-PT (110) substrate with the applied electric field. (c) The dependence of the ZFC magnetic hysteresis loops along the [1 – 10] direction upon the applied electric fields. (d) The electric field dependence of the HC extracted from the hysteresis loops in (c).
    Fig. 2. (a) The ZFC magnetic hysteresis loops measured with magnetic fields applied along the [1 – 10] and [001] directions. (b) A schematic of the strain induced in the PMN-PT (110) substrate with the applied electric field. (c) The dependence of the ZFC magnetic hysteresis loops along the [1 – 10] direction upon the applied electric fields. (d) The electric field dependence of the HC extracted from the hysteresis loops in (c).
    (a) Angular dependence of hysteresis loops of the CoO1–δ/Co bilayer. (b) The extracted HE and HC as functions of the angle. (c) and (d) The angular dependence of the hysteresis loops and the extracted HE(C) calculated with the M–B model.
    Fig. 3. (a) Angular dependence of hysteresis loops of the CoO1–δ/Co bilayer. (b) The extracted HE and HC as functions of the angle. (c) and (d) The angular dependence of the hysteresis loops and the extracted HE(C) calculated with the M–B model.
    The voltage dependence of hysteresis loops after the FC procedure along (a), (b) the [1 – 10] direction and (c), (d) the [001] direction. The hysteresis loops at positive voltages show similar behavior with those at negative voltages.
    Fig. 4. The voltage dependence of hysteresis loops after the FC procedure along (a), (b) the [1 – 10] direction and (c), (d) the [001] direction. The hysteresis loops at positive voltages show similar behavior with those at negative voltages.
    Xin Wen, Rui Wu, Wen-Yun Yang, Chang-Sheng Wang, Shun-Quan Liu, Jing-Zhi Han, Jin-Bo Yang. Room-temperature electric control of exchange bias effect in CoO1 – δ/Co films using Pb(Mg1/3Nb2/3)0.7Ti0.3O3 (110) substrates[J]. Chinese Physics B, 2020, 29(9):
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