Phase Transitions In High-Strain (111)-Cut Pb(Mg1/3Nb2/3)0.7Ti0.3O3 Crystal

碩士 === 輔仁大學 === 物理學系 === 96 === Abstract Phase transformations of the (111)-cut Pb(Mg1/3Nb2/3)0.70Ti0.30O3 single crystals before and after an electric E-field poling have been investigated by means of dielectric permittivity, hysteresis loop, polarization current, and in situ x-ray diffraction...

Full description

Bibliographic Details
Main Authors: Chuang Hui-Tsung, 莊惠宗
Other Authors: Tu Chi-Shun
Format: Others
Language:zh-TW
Published: 2008
Online Access:http://ndltd.ncl.edu.tw/handle/07481749275774994880
id ndltd-TW-096FJU00198010
record_format oai_dc
spelling ndltd-TW-096FJU001980102015-11-30T04:02:35Z http://ndltd.ncl.edu.tw/handle/07481749275774994880 Phase Transitions In High-Strain (111)-Cut Pb(Mg1/3Nb2/3)0.7Ti0.3O3 Crystal 高應變(111)切向Pb(Mg1/3Nb2/3)0.70Ti0.30O3單晶的相轉變 Chuang Hui-Tsung 莊惠宗 碩士 輔仁大學 物理學系 96 Abstract Phase transformations of the (111)-cut Pb(Mg1/3Nb2/3)0.70Ti0.30O3 single crystals before and after an electric E-field poling have been investigated by means of dielectric permittivity, hysteresis loop, polarization current, and in situ x-ray diffraction as a function of temperature. An R-T-C transition sequence was observed in the unpoled sample upon zero-field heating. R, T, and C are rhombohedral, tetragonal, and cubic phases, respectively. After a prior E-field poling, an extra intermediate monoclinic (possible MA) phase was induced and the crystal underwent an R-MA-T-C phase sequence with significant responses in polarization current. The dielectric dispersion was diminished after poling and reappeared in the cubic state. The dielectric permittivities with and without a prior poling were found to follow the Curie-Weiss equation, =C/(T-To), above the Burns temperature 505 K with the same Curie-Weiss constant C=1.9´105 K and Curie-Weiss temperature To=460 K. Tu Chi-Shun 杜繼舜 2008 學位論文 ; thesis 54 zh-TW
collection NDLTD
language zh-TW
format Others
sources NDLTD
description 碩士 === 輔仁大學 === 物理學系 === 96 === Abstract Phase transformations of the (111)-cut Pb(Mg1/3Nb2/3)0.70Ti0.30O3 single crystals before and after an electric E-field poling have been investigated by means of dielectric permittivity, hysteresis loop, polarization current, and in situ x-ray diffraction as a function of temperature. An R-T-C transition sequence was observed in the unpoled sample upon zero-field heating. R, T, and C are rhombohedral, tetragonal, and cubic phases, respectively. After a prior E-field poling, an extra intermediate monoclinic (possible MA) phase was induced and the crystal underwent an R-MA-T-C phase sequence with significant responses in polarization current. The dielectric dispersion was diminished after poling and reappeared in the cubic state. The dielectric permittivities with and without a prior poling were found to follow the Curie-Weiss equation, =C/(T-To), above the Burns temperature 505 K with the same Curie-Weiss constant C=1.9´105 K and Curie-Weiss temperature To=460 K.
author2 Tu Chi-Shun
author_facet Tu Chi-Shun
Chuang Hui-Tsung
莊惠宗
author Chuang Hui-Tsung
莊惠宗
spellingShingle Chuang Hui-Tsung
莊惠宗
Phase Transitions In High-Strain (111)-Cut Pb(Mg1/3Nb2/3)0.7Ti0.3O3 Crystal
author_sort Chuang Hui-Tsung
title Phase Transitions In High-Strain (111)-Cut Pb(Mg1/3Nb2/3)0.7Ti0.3O3 Crystal
title_short Phase Transitions In High-Strain (111)-Cut Pb(Mg1/3Nb2/3)0.7Ti0.3O3 Crystal
title_full Phase Transitions In High-Strain (111)-Cut Pb(Mg1/3Nb2/3)0.7Ti0.3O3 Crystal
title_fullStr Phase Transitions In High-Strain (111)-Cut Pb(Mg1/3Nb2/3)0.7Ti0.3O3 Crystal
title_full_unstemmed Phase Transitions In High-Strain (111)-Cut Pb(Mg1/3Nb2/3)0.7Ti0.3O3 Crystal
title_sort phase transitions in high-strain (111)-cut pb(mg1/3nb2/3)0.7ti0.3o3 crystal
publishDate 2008
url http://ndltd.ncl.edu.tw/handle/07481749275774994880
work_keys_str_mv AT chuanghuitsung phasetransitionsinhighstrain111cutpbmg13nb2307ti03o3crystal
AT zhuānghuìzōng phasetransitionsinhighstrain111cutpbmg13nb2307ti03o3crystal
AT chuanghuitsung gāoyīngbiàn111qièxiàngpbmg13nb23070ti030o3dānjīngdexiāngzhuǎnbiàn
AT zhuānghuìzōng gāoyīngbiàn111qièxiàngpbmg13nb23070ti030o3dānjīngdexiāngzhuǎnbiàn
_version_ 1718139626197090304