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首页> 外文期刊>Physical review >Magnetoelectric coupling in the mixed erythrosiderite [(NH_4)_(1-x)K_x]_2[FeCl_5(H_2O)]
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Magnetoelectric coupling in the mixed erythrosiderite [(NH_4)_(1-x)K_x]_2[FeCl_5(H_2O)]

机译:混合红细胞岩中的磁电耦合[(NH_4)_(1-x)K_X] _2 [FECL_5(H_2O)]

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摘要

We present a study of the dielectric, structural, and magnetic properties of the multiferroic or linear magnetoelectric substitution series [(NH_4)_(1-x)K_x]_2[FeCl_5(H_2O)]. Pyroelectric currents, magnetic susceptibilities, and thermodynamic properties were examined on large single crystals of the erythrosiderite compounds and detailed magnetic-field versus temperature phase diagrams are derived for three different substitution levels. With increasing potassium concentration the material is tuned from a multiferroic (x ≤ 0.06) to a linear magnetoelectric (x ≥ 0.15) ground state. In contrast to the respective pure parent compounds with x = 0 or 1, however, the ferroelectric or linear magnetoelectric polarization in none of the substituted samples is switchable by external electric fields because these samples exhibit a significant electric polarization already above the magnetic ordering transition. The polarization arises at a higher-lying structural phase transition that is examined by THz spectroscopy, and, on a deuterated pure single crystal, by comprehensive neutron-diffraction experiments. The structural phase transition is attributed to an ordering of NH_4~+ tetrahedra but does not break inversion symmetry in the pure material, while a finite K content causes pyroelectricity.
机译:我们介绍了多体型或线性磁电取代串的电介质,结构和磁性序列[(NH_4)_(1-X)K_X] _2 [FECL_5(H_2O)]的研究。在赤藓糖石化合物的大单晶上检查热电电流,磁性敏感性和热力学性质,并导出了三种不同的替代水平的详细磁场与温度相图。随着钾浓度的增加,材料从多体(x≤0.06)从多重(x≤0.06)调谐到线性磁电(x≥0.15)地面状态。然而,与具有X = 0或1的各自的纯母体化合物相反,在没有替代样品中的任何替代样品中的铁电或线性磁电偏振都是由外部电场切换的,因为这些样品已经表现出已经高于磁性有序转变的显着电极化。通过综合中子衍射实验,通过THz光谱检查的高于柔和的结构相转变,并在氘代纯单晶上进行偏振。结构相转变归因于NH_4〜+ Tetrahedra的排序,但在纯材料中不会破坏反转对称性,而有限的K含量导致热电。

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  • 来源
    《Physical review 》 |2020年第5期| 054413.1-054413.11| 共11页
  • 作者单位

    Ⅱ.Physikalisches Institut Universitaet zu Koeln Zuelpicher Strasse 77 50937 Koeln Germany;

    Ⅱ.Physikalisches Institut Universitaet zu Koeln Zuelpicher Strasse 77 50937 Koeln Germany;

    Ⅱ.Physikalisches Institut Universitaet zu Koeln Zuelpicher Strasse 77 50937 Koeln Germany;

    Ⅱ.Physikalisches Institut Universitaet zu Koeln Zuelpicher Strasse 77 50937 Koeln Germany;

    RWTH Aachen University Institut fuer Kristallographie 52056 Aachen Germany Juelich Centre for Neutron Science JCNS at Heinz Maier-Leibnitz Zentrum (MLZ) Forschungszentrum Juelich GmbH Lichtenbergstrasse 1 85747 Garching Germany;

    Abteilung Kristallographie Institut fuer Geologie und Mineralogie Universitaet zu Koeln Zuelpicher Strasse 49b 50674 Koeln Germany;

    Abteilung Kristallographie Institut fuer Geologie und Mineralogie Universitaet zu Koeln Zuelpicher Strasse 49b 50674 Koeln Germany;

    Ⅱ.Physikalisches Institut Universitaet zu Koeln Zuelpicher Strasse 77 50937 Koeln Germany;

    Ⅱ.Physikalisches Institut Universitaet zu Koeln Zuelpicher Strasse 77 50937 Koeln Germany;

    Ⅱ.Physikalisches Institut Universitaet zu Koeln Zuelpicher Strasse 77 50937 Koeln Germany;

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