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固溶体 BiFeO3-BiMnO3 中磁化反转和交换偏置现象的起源:是本征的还是外禀的?

Origin of magnetization reversal and exchange bias phenomena in solid solutions of BiFeO3-BiMnO3: intrinsic or extrinsic?

机构信息

International Center for Materials Nanoarchitectonics (WPI-MANA), National Institute for Materials Science, Namiki 1-1, Tsukuba, Ibaraki, 305-0044, Japan.

出版信息

Inorg Chem. 2013 Feb 18;52(4):2015-21. doi: 10.1021/ic302384j. Epub 2013 Jan 31.

Abstract

Magnetic properties of BiFe(0.7)Mn(0.3)O(3) (with a Néel temperature (T(N)) of 425 K) and BiFe(0.6)Mn(0.4)O(3) (with T(N) = 350 K) were investigated by magnetic measurements between 5 and 400 K. They crystallize in space group Pnma with the √2a(p) × 4a(p) × 2√2a(p) superstructure (a(p) is the parameter of the cubic perovskite subcell) with a = 5.57800(9) Å, b = 15.7038(3) Å, and c = 11.22113(16) Å for BiFe(0.6)Mn(0.4)O(3). Both compounds show magnetization reversal or negative magnetization phenomena. However, it was found that the magnetization reversal is dependent on magnetic prehistory of a sample and measurement protocols. No magnetization reversal was observed when virgin samples were measured below T(N). Magnetization reversal effects appeared only when the samples were cooled in small magnetic fields from temperatures above T(N) or after the samples were magnetized. The exchange bias effect or a shift of isothermal magnetization curves, depending on the measurement conditions, was also observed. The exchange bias changes its sign as a function of temperature and cooling conditions. Our findings allowed us to propose the extrinsic origin (related to sample inhomogeneities) of the magnetization reversal effect in these two compounds.

摘要

通过在 5 到 400 K 之间的磁性测量,研究了 BiFe(0.7)Mn(0.3)O(3)(具有 425 K 的尼尔温度 (T(N)))和 BiFe(0.6)Mn(0.4)O(3)(具有 T(N) = 350 K)的磁性。它们在空间群 Pnma 中结晶,具有 √2a(p) × 4a(p) × 2√2a(p)超结构(a(p) 是立方钙钛矿亚晶格的参数),a(p) = 5.57800(9) Å, b = 15.7038(3) Å, 和 c = 11.22113(16) Å,BiFe(0.6)Mn(0.4)O(3)。这两种化合物都表现出磁化反转或负磁化现象。然而,发现磁化反转取决于样品的磁历史和测量协议。在低于 T(N) 的温度下测量原始样品时,未观察到磁化反转。仅当样品在高于 T(N)的温度下或在样品磁化后在小磁场中冷却时,才会出现磁化反转效应。还观察到交换偏置效应或等温磁化曲线的偏移,这取决于测量条件。交换偏置的符号随温度和冷却条件而变化。我们的发现使我们能够提出这两种化合物中磁化反转效应的外源性起源(与样品不均匀性有关)。

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