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首页> 外文期刊>Journal of Applied Physics >Dielectric, magnetic, and lattice dynamics properties of Y-type hexaferrite Ba_(0.5)Sr_(1.5)Zn_2Fe_(12)O_(22): Comparison of ceramics and single crystals
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Dielectric, magnetic, and lattice dynamics properties of Y-type hexaferrite Ba_(0.5)Sr_(1.5)Zn_2Fe_(12)O_(22): Comparison of ceramics and single crystals

机译:Y型六方铁氧体Ba_(0.5)Sr_(1.5)Zn_2Fe_(12)O_(22)的介电,磁和晶格动力学性质:陶瓷和单晶的比较

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摘要

We prepared multiferroic Y-type hexaferrite Ba_(0.5)Sr_(1.5)Zn_2Fe_(12)O_(22) ceramics and compared their magnetic and dielectric properties with single crystal. Magnetic susceptibility and microwave resonance measurement revealed magnetic phase transition at T_C=312 K, similar as in single crystal. Ferroelectric (FE) phase can be induced by external magnetic field in all investigated samples and the phase diagram in ceramics qualitatively resembles that of the single crystal. The range of magnetic fields, where the FE phase is induced, broadens after annealing of single crystal. Ceramics quenched after sintering exhibit several orders of magnitude lower conductivity than the single crystal. Heavily damped magnetic resonance was discovered in terahertz spectra at 10 K and its frequency softens below 5 GHz near T_C. Number and symmetry of observed infrared (IR) and Raman active phonons correspond to paraelectric phase with D_(3d)~5 hexagonal structure. No evidence for a structural phase transition was found in the IR and Raman spectra on cooling (in zero magnetic field) or in the room-temperature IR spectra with external static magnetic field up to 0.3 T.
机译:我们制备了多铁性Y型六方铁氧体Ba_(0.5)Sr_(1.5)Zn_2Fe_(12)O_(22)陶瓷,并将其磁性能和介电性能与单晶进行了比较。磁化率和微波共振测量表明,在T_C = 312 K时,磁性相变类似于单晶。所有研究样品中的外部磁场均可感应出铁电(FE)相,并且陶瓷中的相图在质量上与单晶相类似。在单晶退火之后,感应出FE相的磁场范围变宽。烧结后淬火的陶瓷的导电率比单晶低几个数量级。在10 K的太赫兹频谱中发现了严重衰减的磁共振,其频率在T_C附近低于5 GHz时变软。观察到的红外和拉曼活性声子的数量和对称性对应于具有D_(3d)〜5六方结构的顺电相。在冷却(在零磁场中)的IR和拉曼光谱中,或在外部静磁场高达0.3 T的室温IR光谱中,未发现结构相变的证据。

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  • 来源
    《Journal of Applied Physics》 |2010年第10期|P.104109.1-104109.7|共7页
  • 作者单位

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Physics, ASCR, Na Slovance 2, 18221 Prague 8, Czech Republic;

    Institute of Inorganic Chemistry, ASCR, 25068 Rez, Czech Republic;

    Division of Materials Physics, Graduate School of Engineering Science, Osaka University, Toyonaka,Osaka 560-8531, Japan;

    Division of Materials Physics, Graduate School of Engineering Science, Osaka University, Toyonaka,Osaka 560-8531, Japan;

    Faculty of Mathematics and Physics, Charles University, V Holesovickach 2, 180 00 Prague 8, Czech Republic;

    Faculty of Mathematics and Physics, Charles University, V Holesovickach 2, 180 00 Prague 8, Czech Republic;

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