Dielectric properties depend on the crystal structure of perovskite-type RbTaO<sub>3</sub> synthesized at high pressure

We successfully synthesized perovskite-type RbTaO<sub>3</sub> at 1173 K under 4 GPa. RbTaO<sub>3</sub> crystalized as a cubic system (<i>Pm</i>3̄<i>m</i> space group (SG), <i>a</i> = 4.04108(3) Å) at 300 K in contrast to the orthorhombic perovskite-type RbNbO<sub>3</sub> prepared under the same conditions. During the cooling process, it reversibly transformed into a tetragonal phase (SG: <i>P</i>4<i>mm</i>) at 270 K, and into an orthorhombic phase (SG: <i>Amm</i>2) at 80 K. Corresponding to the phase transition, the relative permittivity showed a peak at 270 K with a maximum value of approximately 2000 and a kink at 80 K. This transition scheme is analogous to well-known displacement-type ferroelectrics of BaTiO<sub>3</sub> and KNbO<sub>3</sub>. This is in contrast to KTaO<sub>3</sub>, which retains a cubic system and quantum paraelectric properties at the lowest temperature.

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Publication Details

Journal
Dalton Transactions
Published
2025-01-01
DOI
https://doi.org/10.1039/d4dt03207a
Primary Topic
Ferroelectric and Piezoelectric Materials
Type
article
Field-Weighted Citation Impact
0.00

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article

Dielectric properties depend on the crystal structure of perovskite-type RbTaO3 synthesized at high pressure

Jun‐ichi Yamaura, A. Yamamoto, Hajime Sagayama, Yosuke Hamasaki et al.
Dalton Transactions
Ferroelectric and Piezoelectric Materials
article

Dielectric properties depend on the crystal structure of perovskite-type RbTaO3 synthesized at high pressure

Jun‐ichi Yamaura, A. Yamamoto, Hajime Sagayama, Yosuke Hamasaki, Takeharu Kato, K. Murase
article en

Abstract

We successfully synthesized perovskite-type RbTaO<sub>3</sub> at 1173 K under 4 GPa. RbTaO<sub>3</sub> crystalized as a cubic system (<i>Pm</i>3̄<i>m</i> space group (SG), <i>a</i> = 4.04108(3) Å) at 300 K in contrast to the orthorhombic perovskite-type RbNbO<sub>3</sub> prepared under the same conditions. During the cooling process, it reversibly transformed into a tetragonal phase (SG: <i>P</i>4<i>mm</i>) at 270 K, and into an orthorhombic phase (SG: <i>Amm</i>2) at 80 K. Corresponding to the phase transition, the relative permittivity showed a peak at 270 K with a maximum value of approximately 2000 and a kink at 80 K. This transition scheme is analogous to well-known displacement-type ferroelectrics of BaTiO<sub>3</sub> and KNbO<sub>3</sub>. This is in contrast to KTaO<sub>3</sub>, which retains a cubic system and quantum paraelectric properties at the lowest temperature.

Dalton TransactionsVol. 54(6)
National Defence Academy (IN), High Energy Accelerator Research Organization (JP), Shibaura Institute of Technology (JP), Japan Fine Ceramics Center (JP), National Defense Academy of Japan (JP), The University of Tokyo (JP)
University of Tokyo, Institute for Materials Research, Tohoku University, Division of Materials Research
Openalex Percentile: Top 100%
Ferroelectric and Piezoelectric Materials
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Dielectric properties depend on the crystal structure of perovskite-type RbTaO<sub>3</sub> synthesized at high pressure — Jun‐ichi Yamaura, A. Yamamoto, et al. · Dalton Transactions (2025) | TGRS Research Map | TGRS