Effects of Gd<sup>3+</sup> doping on structural and dielectric properties of PZT (Zr:Ti = 52:48) piezoceramics

The purpose of this research is to study the effect of doping Gd into Pb(Zr0.52Ti0.48)O3 ceramics prepared by solid state reaction. X-ray diffraction patterns show that all PGZT samples are of tetragonal structure and the highest doping should be no more than 2 mole∈% Gd at which the unreacted oxide...

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Main Authors: L. Pdungsap, S. Boonyeun, P. Winotai, N. Udomkan, P. Limsuwan
Other Authors: Mahidol University
Format: Article
Published: 2018
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Online Access:https://repository.li.mahidol.ac.th/handle/123456789/16623
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spelling th-mahidol.166232018-06-21T15:35:12Z Effects of Gd<sup>3+</sup> doping on structural and dielectric properties of PZT (Zr:Ti = 52:48) piezoceramics L. Pdungsap S. Boonyeun P. Winotai N. Udomkan P. Limsuwan Mahidol University Thammasat University King Mongkuts University of Technology Thonburi Materials Science Physics and Astronomy The purpose of this research is to study the effect of doping Gd into Pb(Zr0.52Ti0.48)O3 ceramics prepared by solid state reaction. X-ray diffraction patterns show that all PGZT samples are of tetragonal structure and the highest doping should be no more than 2 mole∈% Gd at which the unreacted oxides start to appear. The electron spin resonance (ESR) spectra of PGZT's indicate that Gd3+ can enter both A site of the perovskite structure instead of only A site as widely believed. The ESR peaks resonance shift towards low fields as the concentration is higher, which is due to the change in crystal field experienced by Gd3+ ions. At x =0.001, 0.005 and 0.01 dopings, two sets of powder ESR signals arising from Gd3+ (4f7, spin 7/2) ions at A site. The first set shows some fine structure having strong absorption peaks centered at 76.26 mT (g = 8.550). The second is a seven-peak spectrum centered at 206.01 mT (g = 3.165), which belongs to the Gd3+ ions at B sites. Furthermore, the overlapped ESR strong absorption peaks from 309.17 mT to 314.49 mT (g = 2.2818-2.1087) belong to Gd3+ of unreacted Gd2O 3. The local environments of Gd3+ ions were verified from the calculated ESR spectra using appropriate spin Hamiltonian parameter, i.e. gyromagnetic tensor g, zero-field splitting D and hyperfine tensor A. 2018-06-21T08:17:46Z 2018-06-21T08:17:46Z 2005-12-01 Article European Physical Journal B. Vol.48, No.3 (2005), 367-372 10.1140/epjb/e2005-00407-9 14346036 14346028 2-s2.0-29344465424 https://repository.li.mahidol.ac.th/handle/123456789/16623 Mahidol University SCOPUS https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=29344465424&origin=inward
institution Mahidol University
building Mahidol University Library
continent Asia
country Thailand
Thailand
content_provider Mahidol University Library
collection Mahidol University Institutional Repository
topic Materials Science
Physics and Astronomy
spellingShingle Materials Science
Physics and Astronomy
L. Pdungsap
S. Boonyeun
P. Winotai
N. Udomkan
P. Limsuwan
Effects of Gd<sup>3+</sup> doping on structural and dielectric properties of PZT (Zr:Ti = 52:48) piezoceramics
description The purpose of this research is to study the effect of doping Gd into Pb(Zr0.52Ti0.48)O3 ceramics prepared by solid state reaction. X-ray diffraction patterns show that all PGZT samples are of tetragonal structure and the highest doping should be no more than 2 mole∈% Gd at which the unreacted oxides start to appear. The electron spin resonance (ESR) spectra of PGZT's indicate that Gd3+ can enter both A site of the perovskite structure instead of only A site as widely believed. The ESR peaks resonance shift towards low fields as the concentration is higher, which is due to the change in crystal field experienced by Gd3+ ions. At x =0.001, 0.005 and 0.01 dopings, two sets of powder ESR signals arising from Gd3+ (4f7, spin 7/2) ions at A site. The first set shows some fine structure having strong absorption peaks centered at 76.26 mT (g = 8.550). The second is a seven-peak spectrum centered at 206.01 mT (g = 3.165), which belongs to the Gd3+ ions at B sites. Furthermore, the overlapped ESR strong absorption peaks from 309.17 mT to 314.49 mT (g = 2.2818-2.1087) belong to Gd3+ of unreacted Gd2O 3. The local environments of Gd3+ ions were verified from the calculated ESR spectra using appropriate spin Hamiltonian parameter, i.e. gyromagnetic tensor g, zero-field splitting D and hyperfine tensor A.
author2 Mahidol University
author_facet Mahidol University
L. Pdungsap
S. Boonyeun
P. Winotai
N. Udomkan
P. Limsuwan
format Article
author L. Pdungsap
S. Boonyeun
P. Winotai
N. Udomkan
P. Limsuwan
author_sort L. Pdungsap
title Effects of Gd<sup>3+</sup> doping on structural and dielectric properties of PZT (Zr:Ti = 52:48) piezoceramics
title_short Effects of Gd<sup>3+</sup> doping on structural and dielectric properties of PZT (Zr:Ti = 52:48) piezoceramics
title_full Effects of Gd<sup>3+</sup> doping on structural and dielectric properties of PZT (Zr:Ti = 52:48) piezoceramics
title_fullStr Effects of Gd<sup>3+</sup> doping on structural and dielectric properties of PZT (Zr:Ti = 52:48) piezoceramics
title_full_unstemmed Effects of Gd<sup>3+</sup> doping on structural and dielectric properties of PZT (Zr:Ti = 52:48) piezoceramics
title_sort effects of gd<sup>3+</sup> doping on structural and dielectric properties of pzt (zr:ti = 52:48) piezoceramics
publishDate 2018
url https://repository.li.mahidol.ac.th/handle/123456789/16623
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