Two Types of Negative Thermal Expansion Observed in PbCr1–xTixO3
Source abstract
Abstract
Two negative thermal expansions (NTEs) with different mechanisms were observed in solid solutions of perovskite-type oxides PbCrO 3 and PbTiO 3 . PbCr 1– x Ti x O 3 was found to adopt a cubic structure the same as that of PbCrO 3 for x ≤ 0.6 and a PbTiO 3 -type tetragonal structure for x ≥ 0.7. The NTE observed at x ≤ 0.6 was accompanied by a cubic-to-cubic phase transition originating from the rearrangement of Pb 2+ /Pb 4+ in a complex local structure called a charge glass. The volume shrinkage of −2.5% observed in PbCrO 3 is sufficiently large despite the absence of intermetallic charge transfer, which is the origin of pressure-induced cubic-to-cubic phase transition and 9.8% volume collapse. The NTE in the tetragonal phase was caused by the ferroelectric-to-paraelectric phase transition, the same as in PbTiO 3 . We succeeded in significantly lowering the working temperature of PbTiO 3 as an NTE material by Cr substitution while retaining a large volume shrinkage of 0.6%.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Thermal Expansion and Ionic Conductivity · Ferroelectric and Piezoelectric Materials · Microwave Dielectric Ceramics Synthesis
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Kanagawa Institute of Industrial Science and Technology (KISTEC), Ebina 243-0435, Japan
Laboratory for Materials and Structures, Tokyo Institute of Technology, Yokohama 226-8503, Japan
Funding
Japan Society for the Promotion of Science · Kanagawa Institute of Industrial Science and Technology
References (41)
Show source-provided references
1. 10.1016/0025-5416(87)90523-410.1016/0025-5416(87)90523-4 ↗
2. 10.1021/ic980253h10.1021/ic980253h ↗
3. 10.1088/0953-8984/17/4/R0310.1088/0953-8984/17/4/R03 ↗
4. 10.1088/1468-6996/13/1/01300110.1088/1468-6996/13/1/013001 ↗
5. 10.1039/C4CS00461B10.1039/C4CS00461B ↗
6. 10.1016/j.pmatsci.2017.10.00210.1016/j.pmatsci.2017.10.002 ↗
7. 10.3389/fchem.2018.0037110.3389/fchem.2018.00371 ↗
8. 10.1038/ncomms136110.1038/ncomms1361 ↗
9. 10.1063/1.490825810.1063/1.4908258 ↗
10. 10.1021/acs.chemmater.6b0116010.1021/acs.chemmater.6b01160 ↗
11. 10.7567/APEX.11.06110210.7567/APEX.11.061102 ↗
12. 10.1063/1.481797610.1063/1.4817976 ↗
13. 10.1103/PhysRevB.88.01411210.1103/PhysRevB.88.014112 ↗
14. 10.1021/acs.chemmater.9b0092910.1021/acs.chemmater.9b00929 ↗
15. 10.1103/PhysRevLett.110.11590110.1103/PhysRevLett.110.115901 ↗
16. 10.1063/1.234727910.1063/1.2347279 ↗
17. 10.1039/C6TC03939A10.1039/C6TC03939A ↗
18. 10.1021/jacs.7b0862510.1021/jacs.7b08625 ↗
19. 10.1002/anie.20180408210.1002/anie.201804082 ↗
20. 10.1021/acs.chemmater.0c0170910.1021/acs.chemmater.0c01709 ↗
21. 10.2109/jcersj2.2205910.2109/jcersj2.22059 ↗
22. 10.1021/acs.inorgchem.1c0396010.1021/acs.inorgchem.1c03960 ↗
23. 10.1038/nature0781610.1038/nature07816 ↗
24. 10.1063/1.490389010.1063/1.4903890 ↗
25. 10.1002/anie.20110222810.1002/anie.201102228 ↗
26. 10.1103/PhysRevLett.101.20590110.1103/PhysRevLett.101.205901 ↗
27. 10.1063/1.214772610.1063/1.2147726 ↗
28. 10.1038/ncomms1410210.1038/ncomms14102 ↗
29. 10.1021/acs.chemmater.1c0161910.1021/acs.chemmater.1c01619 ↗
30. 10.1021/ja507748710.1021/ja5077487 ↗
31. 10.1103/PhysRevLett.107.19550410.1103/PhysRevLett.107.195504 ↗
32. 10.1039/b206022a10.1039/b206022a ↗
33. 10.1021/jacs.5b0821610.1021/jacs.5b08216 ↗
34. 10.7567/JJAP.57.05030110.7567/JJAP.57.050301 ↗
35. 10.1103/PhysRev.80.110510.1103/PhysRev.80.1105 ↗
36. 10.1021/ic200680u10.1021/ic200680u ↗
37. 10.1016/S0168-9002(01)00639-810.1016/S0168-9002(01)00639-8 ↗
38. 10.1063/1.499945410.1063/1.4999454 ↗
39. 10.4028/www.scientific.net/SSP.130.1510.4028/www.scientific.net/SSP.130.15 ↗
40. 10.1021/acs.inorgchem.1c0046010.1021/acs.inorgchem.1c00460 ↗
41. 10.1021/ic800649a10.1021/ic800649a ↗