首页> 外文期刊>Applied Physics Letters >Phase coexistence and domain configuration in Pb(Mg_(1/3)Nb_(2/3))O_3-0.34PbTiO_3 single crystal revealed by synchrotron-based X-ray diffractive three-dimensional reciprocal space mapping and piezoresponse force microscopy
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Phase coexistence and domain configuration in Pb(Mg_(1/3)Nb_(2/3))O_3-0.34PbTiO_3 single crystal revealed by synchrotron-based X-ray diffractive three-dimensional reciprocal space mapping and piezoresponse force microscopy

机译:Pb(Mg_(1/3)Nb_(2/3))O_3-0.34PbTiO_3单晶的相共存和畴结构

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摘要

The crystalline phases and domain configuration in the morphotropic phase boundary composition Pb(Mg_(1/3)Nb_(2/3))O_3-0.34PbTiO_3 (PMN-0.34PT) single crystal have been investigated by synchrotron-based X-ray 3D Reciprocal Space Mapping (3D-RSM) and Piezoresponse Force Microscopy. The coexistence of tetragonal (T) and monoclinic M_C phases in this PMN-0.34PT single crystal is confirmed. The affiliation of each diffraction spot in the 3D-RSM was identified with the assistance of qualitative simulation. Most importantly, the twinning structure between different domains in such a mixed phase PMN-PT crystal is firmly clarified, and the spatial distribution of different twin domains is demonstrated. In addition, the lattice parameters of T and M_C phases in PMN-0.34PT single crystal as well as the tilting angles of crystal lattices caused by the interfacial lattice mismatch are determined.
机译:通过基于同步加速器的X射线3D研究了同相相界组成Pb(Mg_(1/3)Nb_(2/3))O_3-0.34PbTiO_3(PMN-0.34PT)单晶中的晶相和畴构型相互空间映射(3D-RSM)和压电响应力显微镜。确认了该PMN-0.34PT单晶中四方(T)相和单斜M_C相共存。在定性模拟的帮助下确定了3D-RSM中每个衍射点的隶属关系。最重要的是,这种混合相PMN-PT晶体中不同畴之间的孪生结构得到了明确的阐明,并且证明了不同孪晶畴的空间分布。此外,还确定了PMN-0.34PT单晶中T和M_C相的晶格参数,以及由界面晶格失配引起的晶格倾斜角。

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  • 来源
    《Applied Physics Letters》 |2016年第15期|152905.1-152905.5|共5页
  • 作者单位

    Department of Physics, Condensed Matter Science and Technology Institute, Harbin Institute of Technology, Harbin 150080, China;

    National Synchrotron Radiation Laboratory and CAS Key Laboratory of Materials for Energy Conversion, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Department of Physics, Condensed Matter Science and Technology Institute, Harbin Institute of Technology, Harbin 150080, China;

    National Synchrotron Radiation Laboratory and CAS Key Laboratory of Materials for Energy Conversion, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Department of Physics, Condensed Matter Science and Technology Institute, Harbin Institute of Technology, Harbin 150080, China;

    National Synchrotron Radiation Laboratory and CAS Key Laboratory of Materials for Energy Conversion, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Department of Physics, Condensed Matter Science and Technology Institute, Harbin Institute of Technology, Harbin 150080, China;

    National Synchrotron Radiation Laboratory and CAS Key Laboratory of Materials for Energy Conversion, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA;

    Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA;

    National Synchrotron Radiation Laboratory and CAS Key Laboratory of Materials for Energy Conversion, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Department of Physics, Condensed Matter Science and Technology Institute, Harbin Institute of Technology, Harbin 150080, China,Department of Mathematics and Materials Research Institute, The Pennsylvania State University, University Park, Pennsylvania 16802, USA;

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