Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics
Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the cer...
Ausführliche Beschreibung
Autor*in: |
Hai, Liu [verfasserIn] Bo-Ping, Zhang [verfasserIn] Yu, Pei [verfasserIn] Lei, Zhao [verfasserIn] Kai-sheng, Wang [verfasserIn] Yan-tao, Liu [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2015 |
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Übergeordnetes Werk: |
Enthalten in: Journal of materials research - Berlin : Springer, 1986, 30(2015), 6 vom: 01. März, Seite 782-790 |
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Übergeordnetes Werk: |
volume:30 ; year:2015 ; number:6 ; day:01 ; month:03 ; pages:782-790 |
Links: |
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DOI / URN: |
10.1557/jmr.2015.51 |
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Katalog-ID: |
SPR042939526 |
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520 | |a Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. | ||
700 | 1 | |a Bo-Ping, Zhang |e verfasserin |4 aut | |
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700 | 1 | |a Lei, Zhao |e verfasserin |4 aut | |
700 | 1 | |a Kai-sheng, Wang |e verfasserin |4 aut | |
700 | 1 | |a Yan-tao, Liu |e verfasserin |4 aut | |
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10.1557/jmr.2015.51 doi (DE-627)SPR042939526 (DE-599)SPRjmr.2015.51-e (SPR)jmr.2015.51-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Hai, Liu verfasserin aut Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. Bo-Ping, Zhang verfasserin aut Yu, Pei verfasserin aut Lei, Zhao verfasserin aut Kai-sheng, Wang verfasserin aut Yan-tao, Liu verfasserin aut Enthalten in Journal of materials research Berlin : Springer, 1986 30(2015), 6 vom: 01. März, Seite 782-790 (DE-627)320527026 (DE-600)2015297-8 2044-5326 nnns volume:30 year:2015 number:6 day:01 month:03 pages:782-790 https://dx.doi.org/10.1557/jmr.2015.51 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_165 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2036 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2088 GBV_ILN_2089 GBV_ILN_2093 GBV_ILN_2098 GBV_ILN_2107 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2145 GBV_ILN_2158 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 51.00 ASE AR 30 2015 6 01 03 782-790 |
spelling |
10.1557/jmr.2015.51 doi (DE-627)SPR042939526 (DE-599)SPRjmr.2015.51-e (SPR)jmr.2015.51-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Hai, Liu verfasserin aut Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. Bo-Ping, Zhang verfasserin aut Yu, Pei verfasserin aut Lei, Zhao verfasserin aut Kai-sheng, Wang verfasserin aut Yan-tao, Liu verfasserin aut Enthalten in Journal of materials research Berlin : Springer, 1986 30(2015), 6 vom: 01. März, Seite 782-790 (DE-627)320527026 (DE-600)2015297-8 2044-5326 nnns volume:30 year:2015 number:6 day:01 month:03 pages:782-790 https://dx.doi.org/10.1557/jmr.2015.51 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_165 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2036 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2088 GBV_ILN_2089 GBV_ILN_2093 GBV_ILN_2098 GBV_ILN_2107 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2145 GBV_ILN_2158 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 51.00 ASE AR 30 2015 6 01 03 782-790 |
allfields_unstemmed |
10.1557/jmr.2015.51 doi (DE-627)SPR042939526 (DE-599)SPRjmr.2015.51-e (SPR)jmr.2015.51-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Hai, Liu verfasserin aut Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. Bo-Ping, Zhang verfasserin aut Yu, Pei verfasserin aut Lei, Zhao verfasserin aut Kai-sheng, Wang verfasserin aut Yan-tao, Liu verfasserin aut Enthalten in Journal of materials research Berlin : Springer, 1986 30(2015), 6 vom: 01. März, Seite 782-790 (DE-627)320527026 (DE-600)2015297-8 2044-5326 nnns volume:30 year:2015 number:6 day:01 month:03 pages:782-790 https://dx.doi.org/10.1557/jmr.2015.51 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_165 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2036 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2088 GBV_ILN_2089 GBV_ILN_2093 GBV_ILN_2098 GBV_ILN_2107 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2145 GBV_ILN_2158 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 51.00 ASE AR 30 2015 6 01 03 782-790 |
allfieldsGer |
10.1557/jmr.2015.51 doi (DE-627)SPR042939526 (DE-599)SPRjmr.2015.51-e (SPR)jmr.2015.51-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Hai, Liu verfasserin aut Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. Bo-Ping, Zhang verfasserin aut Yu, Pei verfasserin aut Lei, Zhao verfasserin aut Kai-sheng, Wang verfasserin aut Yan-tao, Liu verfasserin aut Enthalten in Journal of materials research Berlin : Springer, 1986 30(2015), 6 vom: 01. März, Seite 782-790 (DE-627)320527026 (DE-600)2015297-8 2044-5326 nnns volume:30 year:2015 number:6 day:01 month:03 pages:782-790 https://dx.doi.org/10.1557/jmr.2015.51 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_165 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2036 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2088 GBV_ILN_2089 GBV_ILN_2093 GBV_ILN_2098 GBV_ILN_2107 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2145 GBV_ILN_2158 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 51.00 ASE AR 30 2015 6 01 03 782-790 |
allfieldsSound |
10.1557/jmr.2015.51 doi (DE-627)SPR042939526 (DE-599)SPRjmr.2015.51-e (SPR)jmr.2015.51-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Hai, Liu verfasserin aut Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. Bo-Ping, Zhang verfasserin aut Yu, Pei verfasserin aut Lei, Zhao verfasserin aut Kai-sheng, Wang verfasserin aut Yan-tao, Liu verfasserin aut Enthalten in Journal of materials research Berlin : Springer, 1986 30(2015), 6 vom: 01. März, Seite 782-790 (DE-627)320527026 (DE-600)2015297-8 2044-5326 nnns volume:30 year:2015 number:6 day:01 month:03 pages:782-790 https://dx.doi.org/10.1557/jmr.2015.51 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_165 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2036 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2088 GBV_ILN_2089 GBV_ILN_2093 GBV_ILN_2098 GBV_ILN_2107 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2145 GBV_ILN_2158 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 51.00 ASE AR 30 2015 6 01 03 782-790 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR042939526</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220112054645.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">210130s2015 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1557/jmr.2015.51</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR042939526</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)SPRjmr.2015.51-e</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)jmr.2015.51-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">670</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">51.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Hai, Liu</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2015</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. 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Hai, Liu |
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Hai, Liu ddc 670 bkl 51.00 Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics |
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670 ASE 51.00 bkl Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics |
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Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics |
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effects of sintering temperature on structure and properties of by-pt-pmn ternary piezoelectric ceramics |
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Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics |
abstract |
Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. |
abstractGer |
Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. |
abstract_unstemmed |
Abstract 0.7(0.$ 1BiYbO_{3} $-0.$ 9PbTiO_{3} $)-0.3 Pb($ Mg_{1/3} %$ Nb_{2/3} $)$ O_{3} $ (0.7BYPT-0.3PMN) ternary piezoelectric ceramics were prepared by a columbite precursor method. The effects of sintering temperature on the crystalline phase, microstructure, and electrical properties of the ceramics were systematically investigated. There were two phases coexisting in the 0.7BYPT-0.3PMN ceramics sintered at 1100–1250 °C, one is the perovskite host phase with tetragonal symmetry and the other is $ Yb_{2} %$ Ti_{2} %$ O_{7} $ impurity phase. It was observed that, with increasing sintering temperature, the piezoelectric constant d33, dielectric constant $ ε_{r} $, planar electromechanical coupling coefficient kp, and Curie temperature TC increased initially and then decreased. An apparent structure distortion could also be observed in samples synthesized at high sintering temperature due to the severe volatilization of Pb and Bi. The optimum performances of the material were obtained for samples sintered at 1150 °C with d33 = 100 pC/N, $ ε_{r} $ = 494, kp = 25.4%, and TC = 380 °C, respectively. It can be ascribed to the combined effect of a higher density, structural homogeneity with decreased tetragonality as well as a small amount of pyrochlore phase. |
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container_issue |
6 |
title_short |
Effects of sintering temperature on structure and properties of BY-PT-PMN ternary piezoelectric ceramics |
url |
https://dx.doi.org/10.1557/jmr.2015.51 |
remote_bool |
true |
author2 |
Bo-Ping, Zhang Yu, Pei Lei, Zhao Kai-sheng, Wang Yan-tao, Liu |
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Bo-Ping, Zhang Yu, Pei Lei, Zhao Kai-sheng, Wang Yan-tao, Liu |
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doi_str |
10.1557/jmr.2015.51 |
up_date |
2024-07-03T15:41:32.559Z |
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|
score |
7.3998175 |