首页> 外文会议>Annual Conference on Magnetism and Magnetic Materials >(07E128) Magnetic and charge ordering properties of Bi_(0.6-x)(RE)_xCa_(0.4)MnO_3 (0.0 ≤ x ≤ 0.6) perovskite manganites
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(07E128) Magnetic and charge ordering properties of Bi_(0.6-x)(RE)_xCa_(0.4)MnO_3 (0.0 ≤ x ≤ 0.6) perovskite manganites

机译:(07E128)Bi_(0.6-x)(Re)_xCa_(0.4)MnO_3(0.0≤x≤0.6)钙钛矿锰的磁性和电荷排序性能

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In this work, we studied structural, magnetic, and charge ordering properties of polycrystalline Bi_(0.6-x)(RE)_xCa_(0.4)MnO_3 (x = 0.0, 0.1, 0.2, 0.3, 0.4,0.5, and 0.6) samples, synthesized via solid state reaction route and by taking RE = La, Pr, and Nd, separately. The temperature dependence magnetization measurement reveals that the x = 0.0 compound (BCMO) exhibits a charge ordered (CO) and antiferromagnetic (AFM) phase with the charge ordering temperature (T_(CO)) ~289 K and the antiferromagnetic ordering temperature (T_N) ~136 K. Only a small fraction of La-dopant in BCMO is sufficient to destroy the CO completely, whereas a large concentration of La (viz., x = 0.2 to x = 0.6) promotes ultimately a paramagnetic to ferromagnetic (PM-FM) transition, and the PM-FM transition temperature (T_c) decreases progressively from 241K to 203 K as x increases from 0.2 to 0.5. In contrast, systematic substitution of Pr or Nd at Bi site induces an intriguing interplay between the charge ordering and antiferromagnetism. Our results demonstrate that the value of T_(CO) decreases with increasing value of "x" and the value of T_N increases sharply at both the extremes; however, it remains nearly constant from x = 0.2 to 0.4. In our samples, a glassy magnetic states are also observed at far below the T_N.
机译:在这项工作中,我们研究了多晶Bi_(0.6-x)(Re)_xCa_(0.4)MnO_3(x = 0.0,0.1,0.2,0.3,0.4,0.5和0.6)样品的结构,磁性和充电性能。通过固态反应途径合成,并通过单独服用Re = La,Pr和Nd。温度依赖性磁化测量揭示X = 0.0化合物(BCMO)表现出充电有序(CO)和反铁磁(AFM)相位,其中电荷有序温度(T_(CO))〜289k和反铁磁性排序温度(T_N) 〜136 K. BCMO中只有一小部分La-Dopant完全破坏CO,而大量浓度的La(X = 0.2至x = 0.6)促进了铁磁性的顺磁性(PM-FM过渡,PM-FM转变温度(T_C)逐渐从241K到203K降低,因为x从0.2增加到0.5。相反,BI站点的PR或ND系统的替代引起了电荷排序与反铁磁之间的有趣相互作用。我们的结果表明,T_(CO)的值随着“X”的增加而降低,并且T_N的值在极端的两个时急剧增加;但是,它仍然从x = 0.2到0.4几乎恒定。在我们的样品中,在远低于T_N的情况下也观察到玻璃状磁性状态。

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