journal article·2019-08-27

Weak Ferroelectricity in n = 2 Pseudo Ruddlesden–Popper-Type Niobate Li2SrNb2O7

Takayuki Nagai, Hirokazu Shirakuni, Akitoshi Nakano, Hiroshi Sawa, Hiroki Moriwake, Ichiro Terasaki, Hiroki Taniguchi

Chemistry of Materials· Volume 31· Issue 16
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Abstract

Li2SrNb2O7 (LSNO) crystallizes in a structure closely related to n = 2 Ruddlesden–Popper-type compounds, which are generally formed by intergrowth of two-dimensional perovskite-type blocks and rocksalt-type layers. The present study demonstrates the coexistence of spontaneous polarization and an anti-ferroelectric-like nonlinear response in LSNO at 80 K, suggesting weak ferroelectricity below the phase transition temperature of 217 K. A combination of first-principles calculations and single-crystal X-ray diffractions clarifies a polar P21cn structure for the ground state of LSNO, where an in-plane antiferroelectric displacement and an out-of-plane polar shift simultaneously take place. The present study offers a new perspective to design ferroelectric and antiferroelectric materials with Ruddlesden–Popper-type compounds.
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Research context

OpenAlex topics: Ferroelectric and Piezoelectric Materials · Multiferroics and related materials · Microwave Dielectric Ceramics Synthesis

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan

Department of Physics, Nagoya University, Furocho, Chikusaku, Nagoya 464-8602, Japan

Department of Applied Physics, Nagoya University, Furocho, Chikusaku, Nagoya 464-8603, Japan

Nanostructures Research Laboratory, Japan Fine Ceramics Center, 2-4-1 Matsuno, Atsutaku, Nagoya 456-8587, Japan

Funding

Core Research for Evolutional Science and Technology · Japan Society for the Promotion of Science

References (32)

Show source-provided references
1. 10.1111/j.1151-2916.1999.tb01840.x10.1111/j.1151-2916.1999.tb01840.x ↗
2. 10.1088/0960-1317/10/2/30710.1088/0960-1317/10/2/307 ↗
3. 10.1103/PhysRevLett.106.10720410.1103/PhysRevLett.106.107204 ↗
4. 10.1016/j.jssc.2012.04.01210.1016/j.jssc.2012.04.012 ↗
5. 10.1021/jp000114x10.1021/jp000114x ↗
6. 10.1016/0031-9163(66)91127-910.1016/0031-9163(66)91127-9 ↗
7. 10.1103/PhysRevLett.108.13720210.1103/PhysRevLett.108.137202 ↗
8. 10.1021/cr300279n10.1021/cr300279n ↗
9. 10.1002/adma.20160128810.1002/adma.201601288 ↗
10. 10.1021/jacs.8b0799810.1021/jacs.8b07998 ↗
11. 10.1002/adfm.20180185610.1002/adfm.201801856 ↗
12. 10.1021/acs.chemmater.9b0078610.1021/acs.chemmater.9b00786 ↗
13. 10.1107/S010827010101849210.1107/S0108270101018492 ↗
14. 10.1088/0953-8984/16/29/02310.1088/0953-8984/16/29/023 ↗
15. 10.1107/S056774087200797610.1107/S0567740872007976 ↗
16. 10.1039/a904416g10.1039/a904416g ↗
17. 10.1016/j.ceramint.2016.01.12410.1016/j.ceramint.2016.01.124 ↗
18. 10.1103/PhysRevB.51.265110.1103/PhysRevB.51.2651 ↗
19. 10.1080/0015019970801608810.1080/00150199708016088 ↗
20. 10.1063/1.283102310.1063/1.2831023 ↗
21. 10.1103/PhysRevB.50.1795310.1103/PhysRevB.50.17953 ↗
22. 10.1103/PhysRevB.59.175810.1103/PhysRevB.59.1758 ↗
23. 10.1103/PhysRevB.54.1116910.1103/PhysRevB.54.11169 ↗
24. 10.1016/0022-3697(68)90164-910.1016/0022-3697(68)90164-9 ↗
25. Gavrilyachenko V. G. · Sov. Phys. Solid State · 1970 · 12 · 1203
26. 10.1063/1.166261010.1063/1.1662610 ↗
27. 10.1103/PhysRevApplied.7.03401210.1103/PhysRevApplied.7.034012 ↗
28. 10.1038/nature0201810.1038/nature02018 ↗
29. 10.1103/PhysRevLett.108.24760110.1103/PhysRevLett.108.247601 ↗
30. 10.1016/0167-577X(90)90062-Q10.1016/0167-577X(90)90062-Q ↗
31. 10.1002/ange.20130218810.1002/ange.201302188 ↗
32. 10.1103/PhysRevB.98.13410210.1103/PhysRevB.98.134102 ↗