Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary

Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric prop...
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Autor*in:	Wei, Jianxin [verfasserIn] Fu, Dongyan [verfasserIn] Cheng, Jinrong [verfasserIn] Chen, Jianguo [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2017

Übergeordnetes Werk:	Enthalten in: Journal of materials science - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966, 52(2017), 18 vom: 14. Juni, Seite 10726-10737
Übergeordnetes Werk:	volume:52 ; year:2017 ; number:18 ; day:14 ; month:06 ; pages:10726-10737

Links:	Volltext

DOI / URN:	10.1007/s10853-017-1280-6

Katalog-ID:	SPR013924133

Internformat


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520			\|a Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications.
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Indexfelder

author_variant	j w jw d f df j c jc j c jc
matchkey_str	article:15734803:2017----::eprtrdpnecoteilcrcnpeolcrcrprisfbfo3xai_crmcn
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publishDate	2017
allfields	10.1007/s10853-017-1280-6 doi (DE-627)SPR013924133 (SPR)s10853-017-1280-6-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Wei, Jianxin verfasserin aut Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications. Fu, Dongyan verfasserin aut Cheng, Jinrong verfasserin aut Chen, Jianguo verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 18 vom: 14. Juni, Seite 10726-10737 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:18 day:14 month:06 pages:10726-10737 https://dx.doi.org/10.1007/s10853-017-1280-6 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 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_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_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 52 2017 18 14 06 10726-10737
spelling	10.1007/s10853-017-1280-6 doi (DE-627)SPR013924133 (SPR)s10853-017-1280-6-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Wei, Jianxin verfasserin aut Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications. Fu, Dongyan verfasserin aut Cheng, Jinrong verfasserin aut Chen, Jianguo verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 18 vom: 14. Juni, Seite 10726-10737 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:18 day:14 month:06 pages:10726-10737 https://dx.doi.org/10.1007/s10853-017-1280-6 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 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_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_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 52 2017 18 14 06 10726-10737
allfields_unstemmed	10.1007/s10853-017-1280-6 doi (DE-627)SPR013924133 (SPR)s10853-017-1280-6-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Wei, Jianxin verfasserin aut Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications. Fu, Dongyan verfasserin aut Cheng, Jinrong verfasserin aut Chen, Jianguo verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 18 vom: 14. Juni, Seite 10726-10737 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:18 day:14 month:06 pages:10726-10737 https://dx.doi.org/10.1007/s10853-017-1280-6 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 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_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_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 52 2017 18 14 06 10726-10737
allfieldsGer	10.1007/s10853-017-1280-6 doi (DE-627)SPR013924133 (SPR)s10853-017-1280-6-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Wei, Jianxin verfasserin aut Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications. Fu, Dongyan verfasserin aut Cheng, Jinrong verfasserin aut Chen, Jianguo verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 18 vom: 14. Juni, Seite 10726-10737 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:18 day:14 month:06 pages:10726-10737 https://dx.doi.org/10.1007/s10853-017-1280-6 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 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_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_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 52 2017 18 14 06 10726-10737
allfieldsSound	10.1007/s10853-017-1280-6 doi (DE-627)SPR013924133 (SPR)s10853-017-1280-6-e DE-627 ger DE-627 rakwb eng 670 ASE 51.00 bkl Wei, Jianxin verfasserin aut Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications. Fu, Dongyan verfasserin aut Cheng, Jinrong verfasserin aut Chen, Jianguo verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966 52(2017), 18 vom: 14. Juni, Seite 10726-10737 (DE-627)315293969 (DE-600)2015305-3 1573-4803 nnns volume:52 year:2017 number:18 day:14 month:06 pages:10726-10737 https://dx.doi.org/10.1007/s10853-017-1280-6 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 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_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_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 52 2017 18 14 06 10726-10737
language	English
source	Enthalten in Journal of materials science 52(2017), 18 vom: 14. Juni, Seite 10726-10737 volume:52 year:2017 number:18 day:14 month:06 pages:10726-10737
sourceStr	Enthalten in Journal of materials science 52(2017), 18 vom: 14. Juni, Seite 10726-10737 volume:52 year:2017 number:18 day:14 month:06 pages:10726-10737
format_phy_str_mv	Article
institution	findex.gbv.de
dewey-raw	670
isfreeaccess_bool	false
container_title	Journal of materials science
authorswithroles_txt_mv	Wei, Jianxin @@aut@@ Fu, Dongyan @@aut@@ Cheng, Jinrong @@aut@@ Chen, Jianguo @@aut@@
publishDateDaySort_date	2017-06-14T00:00:00Z
hierarchy_top_id	315293969
dewey-sort	3670
id	SPR013924133
language_de	englisch
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XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. 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author	Wei, Jianxin
spellingShingle	Wei, Jianxin ddc 670 bkl 51.00 Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary
authorStr	Wei, Jianxin
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topic_title	670 ASE 51.00 bkl Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary
topic	ddc 670 bkl 51.00
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format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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title	Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary
ctrlnum	(DE-627)SPR013924133 (SPR)s10853-017-1280-6-e
title_full	Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary
author_sort	Wei, Jianxin
journal	Journal of materials science
journalStr	Journal of materials science
lang_code	eng
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container_start_page	10726
author_browse	Wei, Jianxin Fu, Dongyan Cheng, Jinrong Chen, Jianguo
container_volume	52
class	670 ASE 51.00 bkl
format_se	Elektronische Aufsätze
author-letter	Wei, Jianxin
doi_str_mv	10.1007/s10853-017-1280-6
dewey-full	670
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title_sort	temperature dependence of the dielectric and piezoelectric properties of x$ bifeo_{3} $–(1 − x)$ batio_{3} $ ceramics near the morphotropic phase boundary
title_auth	Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary
abstract	Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications.
abstractGer	Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications.
abstract_unstemmed	Abstract Lead-free and high-temperature piezoelectric ceramics of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $-1.0 mol% $ MnO_{2} $ (0.67 ≤ x ≤ 0.78) (xBF–(1 − x)BT-Mn) were fabricated by the conventional solid-state reaction method, and their high-temperature dielectric, piezoelectric and ferroelectric properties near the morphotropic phase boundary were studied systematically. XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications.
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title_short	Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary
url	https://dx.doi.org/10.1007/s10853-017-1280-6
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author2	Fu, Dongyan Cheng, Jinrong Chen, Jianguo
author2Str	Fu, Dongyan Cheng, Jinrong Chen, Jianguo
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doi_str	10.1007/s10853-017-1280-6
up_date	2024-07-03T23:02:59.969Z
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XRD analysis revealed that xBF–(1 − x)BT-Mn ceramics exhibited pure perovskite structure, and the phase was driven by composition variation from the pseudo-cubic (0.67 ≤ x < 0.70) to rhombohedral (0.70 ≤ x ≤ 0.78). The dielectric constant εr (1 kHz), dielectric loss tanδ (1 kHz), Curie temperature TC, depolarization temperature Td, piezoelectric constant d33, remnant polarization Pr (60 kV/cm) and room temperature planar electromechanical coupling factor kp of xBF–(1 − x)BT-Mn ceramics of x = 0.70 were 740, 0.045, 487, 430 °C, 35.5 μC/$ cm^{2} $, 177 pC/N and 0.37, respectively. The unipolar strain and high field strain coefficient d33* of xBF–(1 − x)BT-Mn ceramics with x = 0.70 increased up to 0.26% and 652 pm/V at 180 °C. Temperature dependence of εr, tanδ and kp of xBF–(1 − x)BT-Mn ceramics with x = 0.75 was stable from room temperature even up to 500 °C. These results indicated that xBF–(1 − x)BT-Mn ceramics were promising candidates for high-temperature lead-free piezoelectric applications.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Fu, Dongyan</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Cheng, Jinrong</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Chen, Jianguo</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of materials science</subfield><subfield code="d">Dordrecht [u.a.] : Springer Science + Business Media B.V, 1966</subfield><subfield code="g">52(2017), 18 vom: 14. 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Temperature dependence of the dielectric and piezoelectric properties of x$ BiFeO_{3} $–(1 − x)$ BaTiO_{3} $ ceramics near the morphotropic phase boundary

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