Dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics
The scaling relation of ferroelectric hysteresis area 〈A〉 against frequency f and field amplitude E0 for the saturated loops of the hard lead zirconate titanate bulk ceramic takes the form of 〈A〉 f-0.28 E00.89, while that for the minor loops takes the form of 〈A〉 f-0.43 E03.19. In both cases, the sc...
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th-cmuir.6653943832-52872014-08-30T02:56:22Z Dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics Yimnirun R. Wongmaneerung R. Wongsaenmai S. Ngamjarurojana A. Ananta S. Laosiritaworn Y. The scaling relation of ferroelectric hysteresis area 〈A〉 against frequency f and field amplitude E0 for the saturated loops of the hard lead zirconate titanate bulk ceramic takes the form of 〈A〉 f-0.28 E00.89, while that for the minor loops takes the form of 〈A〉 f-0.43 E03.19. In both cases, the scaling relations are similar to those of its soft counterpart. This indicates that the dynamic behaviors and scaling relations in bulk ceramics are mainly governed by the domain states and structures, while the distinct types of complex defects contribute mainly to the difference in the coercive field observed in hard and soft ceramics. © 2007 American Institute of Physics. 2014-08-30T02:56:22Z 2014-08-30T02:56:22Z 2007 Article 00036951 10.1063/1.2713769 APPLA http://www.scopus.com/inward/record.url?eid=2-s2.0-33947316594&partnerID=40&md5=fac978e874a58547fe5a50b8fd00f4a8 http://cmuir.cmu.ac.th/handle/6653943832/5287 English |
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The scaling relation of ferroelectric hysteresis area 〈A〉 against frequency f and field amplitude E0 for the saturated loops of the hard lead zirconate titanate bulk ceramic takes the form of 〈A〉 f-0.28 E00.89, while that for the minor loops takes the form of 〈A〉 f-0.43 E03.19. In both cases, the scaling relations are similar to those of its soft counterpart. This indicates that the dynamic behaviors and scaling relations in bulk ceramics are mainly governed by the domain states and structures, while the distinct types of complex defects contribute mainly to the difference in the coercive field observed in hard and soft ceramics. © 2007 American Institute of Physics. |
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Article |
author |
Yimnirun R. Wongmaneerung R. Wongsaenmai S. Ngamjarurojana A. Ananta S. Laosiritaworn Y. |
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Yimnirun R. Wongmaneerung R. Wongsaenmai S. Ngamjarurojana A. Ananta S. Laosiritaworn Y. Dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics |
author_facet |
Yimnirun R. Wongmaneerung R. Wongsaenmai S. Ngamjarurojana A. Ananta S. Laosiritaworn Y. |
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Yimnirun R. |
title |
Dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics |
title_short |
Dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics |
title_full |
Dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics |
title_fullStr |
Dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics |
title_full_unstemmed |
Dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics |
title_sort |
dynamic hysteresis and scaling behavior of hard lead zirconate titanate bulk ceramics |
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2014 |
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http://www.scopus.com/inward/record.url?eid=2-s2.0-33947316594&partnerID=40&md5=fac978e874a58547fe5a50b8fd00f4a8 http://cmuir.cmu.ac.th/handle/6653943832/5287 |
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