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Acoustic emission and domain switching in tetragonal lead zirconate titanate ceramics
The electric field-induced acoustic emission (AE) in a poled tetragonal lead zirconate titanate (PZT) ceramic was measured at room temperature and related to the polarization switching, field-induced strain, dielectric constant, and piezoelectric constant in the high-voltage electric field. The AE s...
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Published in: | Japanese Journal of Applied Physics 1994, Vol.33 (9B), p.5555-5558 |
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container_end_page | 5558 |
container_issue | 9B |
container_start_page | 5555 |
container_title | Japanese Journal of Applied Physics |
container_volume | 33 |
creator | SAITO, Y HORI, S |
description | The electric field-induced acoustic emission (AE) in a poled tetragonal lead zirconate titanate (PZT) ceramic was measured at room temperature and related to the polarization switching, field-induced strain, dielectric constant, and piezoelectric constant in the high-voltage electric field. The AE signals became most remarkable when the polarization approached the saturation, while they became minimal when the polarization reversal occurred. The AE count, expressed as a function of electric field, exhibited a hysteresis loop similar to the strain loop. These data suggest that the AE signals were generated by the strain due to 90° domain switching rather than the piezoelectric strain. |
doi_str_mv | 10.1143/jjap.33.5555 |
format | article |
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The AE signals became most remarkable when the polarization approached the saturation, while they became minimal when the polarization reversal occurred. The AE count, expressed as a function of electric field, exhibited a hysteresis loop similar to the strain loop. 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The AE signals became most remarkable when the polarization approached the saturation, while they became minimal when the polarization reversal occurred. The AE count, expressed as a function of electric field, exhibited a hysteresis loop similar to the strain loop. 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The AE signals became most remarkable when the polarization approached the saturation, while they became minimal when the polarization reversal occurred. The AE count, expressed as a function of electric field, exhibited a hysteresis loop similar to the strain loop. These data suggest that the AE signals were generated by the strain due to 90° domain switching rather than the piezoelectric strain.</abstract><cop>Tokyo</cop><pub>Japanese journal of applied physics</pub><doi>10.1143/jjap.33.5555</doi><tpages>4</tpages></addata></record> |
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language | eng |
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source | IOPscience journals; Institute of Physics |
subjects | Acoustical properties of solids Condensed matter: electronic structure, electrical, magnetic, and optical properties Condensed matter: structure, mechanical and thermal properties Dielectric, piezoelectric, ferroelectric and antiferroelectric materials Dielectrics, piezoelectrics, and ferroelectrics and their properties Exact sciences and technology Mechanical and acoustical properties of condensed matter Niobates, titanates, tantalates, pzt ceramics, etc Physics Piezoelectricity and electromechanical effects |
title | Acoustic emission and domain switching in tetragonal lead zirconate titanate ceramics |
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