Polar order in quantum paraelectric SrTi16O3 and SrTi18O3 at low temperature

被引:31
作者
Uesu, Y
Nakai, R
Kiat, JM
Ménoret, C
Itoh, M
Kyomen, T
机构
[1] Waseda Univ, Dept Phys, Shinjuku Ku, Tokyo 1698555, Japan
[2] Waseda Univ, Adv Res Inst Sci & Engn, Shinjuku Ku, Tokyo 1698555, Japan
[3] Ecole Cent Paris, Lab Struct, F-92295 Chatenay Malabry, France
[4] CE Saclay, Leon Brillouin Lab, F-91191 Gif Sur Yvette, France
[5] Tokyo Inst Technol, Mat & Struct Lab, Midori Ku, Yokohama, Kanagawa 2268503, Japan
关键词
quantum paraelectricity; (SrTiO3)-O-16; (SrTiO3)-O-18; polar nanoregion; SHG microscope; x-ray diffraction; neutron powder diffraction;
D O I
10.1143/JPSJ.73.1139
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Optical second-harmonic generation (SHG) in (SrTiO3)-O-16 (STO16) and (SrTiO3)-O-18 (STO18) was investigated using the SHG microscope. While no biased STO16 exhibits weak and almost temperature-independent SHG signals, a marked SHG is observed under the electric field in the quantum paraelectric region. In STO18, strong SHG signals appear spontaneously below 36 K. However, neutron and X-ray diffraction analyses indicate that no structural change appears at low temperature in STO18, or STO16 under the electric field. By taking into account the fact that the SHG is sensitive to the local polar order, the combined studies reveal that the long-range order of the polar phase does not develop on either crystal and is frozen in local regions.
引用
收藏
页码:1139 / 1142
页数:4
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