Structural and electrical properties of BKT rich Bi0.5K0.5TiO3-K0.5Na0.5NbO3 system

A new lead free (1−x) Bi0.5K0.5TiO3–(x) K0.5Na0.5NbO3 (BKT-KNN) system (0.0 ≤ x ≤ 0.15) with density of 94-97% is reported. Tetragonal structure of BKT-KNN is apparent for 0 ≤ x ≤ 0.06 with 1.02 ≤ (c/a) ≤ 1.012. Compositions with x ≥ 0.15 show orthorhombic structure (like KNN) and x = 0.08 & x =...

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Main Authors: Amrita Singh, Ratnamala Chatterjee
Format: Article
Language:English
Published: AIP Publishing LLC 2013-03-01
Series:AIP Advances
Online Access:http://link.aip.org/link/doi/10.1063/1.4796166
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spelling doaj-5f7cf29153c44026bf0f4a7e83c5babc2020-11-24T21:19:20ZengAIP Publishing LLCAIP Advances2158-32262013-03-013303212903212910.1063/1.4796166Structural and electrical properties of BKT rich Bi0.5K0.5TiO3-K0.5Na0.5NbO3 systemAmrita SinghRatnamala ChatterjeeA new lead free (1−x) Bi0.5K0.5TiO3–(x) K0.5Na0.5NbO3 (BKT-KNN) system (0.0 ≤ x ≤ 0.15) with density of 94-97% is reported. Tetragonal structure of BKT-KNN is apparent for 0 ≤ x ≤ 0.06 with 1.02 ≤ (c/a) ≤ 1.012. Compositions with x ≥ 0.15 show orthorhombic structure (like KNN) and x = 0.08 & x = 0.10 are pseudocubic. Addition of KNN by a small amount (up to 4 mole %) is shown to improve piezoelectric properties, keeping the ferroelectric and dielectric values comparable to those of BKT. Optimized properties with d33 = 129 pC/N, kp = 29%, Pmax = 35 μC/cm2, Pr = 24 μC/cm2, ɛm = 4600, Tm = 370 °C and Td = 260 °C are observed for x = 0.03 sample. In the tetragonal range, a correlation between lattice distortion (c/a), piezoelectric coefficient (d33) and depolarization temperature Td is established. Decrease in c/a seems to result in easy poling by field and easy depoling by temperature, leading to an increase in d33 but a decrease in Td. A phase diagram for 1-xBKT-xKNN (0 ≤ x ≤ 0.10) is proposed. It is shown that addition of more than 6 mole % of KNN leads to the lowering of Td (where the structure becomes tetragonal to pseudocubic) considerably, resulting into a shift in tetragonal- pseudocubic phase boundary towards lower temperature.http://link.aip.org/link/doi/10.1063/1.4796166
collection DOAJ
language English
format Article
sources DOAJ
author Amrita Singh
Ratnamala Chatterjee
spellingShingle Amrita Singh
Ratnamala Chatterjee
Structural and electrical properties of BKT rich Bi0.5K0.5TiO3-K0.5Na0.5NbO3 system
AIP Advances
author_facet Amrita Singh
Ratnamala Chatterjee
author_sort Amrita Singh
title Structural and electrical properties of BKT rich Bi0.5K0.5TiO3-K0.5Na0.5NbO3 system
title_short Structural and electrical properties of BKT rich Bi0.5K0.5TiO3-K0.5Na0.5NbO3 system
title_full Structural and electrical properties of BKT rich Bi0.5K0.5TiO3-K0.5Na0.5NbO3 system
title_fullStr Structural and electrical properties of BKT rich Bi0.5K0.5TiO3-K0.5Na0.5NbO3 system
title_full_unstemmed Structural and electrical properties of BKT rich Bi0.5K0.5TiO3-K0.5Na0.5NbO3 system
title_sort structural and electrical properties of bkt rich bi0.5k0.5tio3-k0.5na0.5nbo3 system
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2013-03-01
description A new lead free (1−x) Bi0.5K0.5TiO3–(x) K0.5Na0.5NbO3 (BKT-KNN) system (0.0 ≤ x ≤ 0.15) with density of 94-97% is reported. Tetragonal structure of BKT-KNN is apparent for 0 ≤ x ≤ 0.06 with 1.02 ≤ (c/a) ≤ 1.012. Compositions with x ≥ 0.15 show orthorhombic structure (like KNN) and x = 0.08 & x = 0.10 are pseudocubic. Addition of KNN by a small amount (up to 4 mole %) is shown to improve piezoelectric properties, keeping the ferroelectric and dielectric values comparable to those of BKT. Optimized properties with d33 = 129 pC/N, kp = 29%, Pmax = 35 μC/cm2, Pr = 24 μC/cm2, ɛm = 4600, Tm = 370 °C and Td = 260 °C are observed for x = 0.03 sample. In the tetragonal range, a correlation between lattice distortion (c/a), piezoelectric coefficient (d33) and depolarization temperature Td is established. Decrease in c/a seems to result in easy poling by field and easy depoling by temperature, leading to an increase in d33 but a decrease in Td. A phase diagram for 1-xBKT-xKNN (0 ≤ x ≤ 0.10) is proposed. It is shown that addition of more than 6 mole % of KNN leads to the lowering of Td (where the structure becomes tetragonal to pseudocubic) considerably, resulting into a shift in tetragonal- pseudocubic phase boundary towards lower temperature.
url http://link.aip.org/link/doi/10.1063/1.4796166
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