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The magnetization measurements have shown that the Fe2O3 − X film exhibits ferromagnetic behavior with a remanent magnetization (Mr) of 0.16 memu and coercivity (Hc) of 0.26 kOe.
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The heterostructure exhibited an interesting martensite to austenite phase transformation and polarization-electric field hysteresis behavior with remanent polarization (Pr) and the coercive field (Er) of 17.1 μC/cm2 and 69.6 kV/cm, respectively.
Ferroelectric performance in SiO2-doped HfO2 with a remanent polarization (P r) above 10 μC/cm2 and a coercive field strength (E c) of 1 MV/cm was reported [1].
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It exhibits a ferromagnetic behavior with saturation magnetization (Ms), remanent magnetization (Mr), and coercivity (Hc) values of ca. 71.6 emu/g, 18.4 emu/g, and 152.2 Oe, respectively.
The magnetic characterization of the samples reveals that the samples showed paramagnetic and ferromagnetic behavior, meanwhile there is no linear variation of magnetic moment with concentration of Mn ion whereby at x = 0.15 the samples show room temperature ferromagnetic behavior with coercive field and remanent magnetization of 47.70 Oe and 1.8 × 10−1 emu/g, respectively.
The parallelepiped nanocrystals exhibited a ferromagnetic behavior with the coercive force, saturation magnetization, and remanent magnetization of 920 Oe, 0.44 emu/g, and 0.17 emu/g, respectively.
Two factors: (1) effective confinement of the HfO2 layer by the ZrO2 layer and Si substrate to promote the ferroelectric orthorhombic phase and (2) reduction of the bulk characteristics of the ZrO2 and HfO2 layers to minimize the paraelectric monoclinic phase are the key to stable ferroelectricity with a large remanent polarization.
For the wires after stress-annealing at variable temperatures we obtained a graded magnetic behavior with local hysteresis loops shapes and features (coercivity, remanent magnetization) changing along the sample length.
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