Tuning electrical heterogeneity in CaCu

Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strateg...
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Gespeichert in:

Autor*in:	Mao, Pu [verfasserIn] Zeng, Congbin [verfasserIn] Guo, Yongguang [verfasserIn] Lu, Gang [verfasserIn] Yan, Qingsong [verfasserIn] Liu, Zhiyong [verfasserIn] Xie, Bing [verfasserIn] Zhao, Yingying [verfasserIn] Guo, Kun [verfasserIn] Zhang, Lixue [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2023

Schlagwörter:	CCTO ceramics Dielectric properties Nonlinear characteristics Electrical heterogeneity Nano ZnO

Übergeordnetes Werk:	Enthalten in: Materials research bulletin - New York, NY [u.a.] : Elsevier, 1966, 164
Übergeordnetes Werk:	volume:164

DOI / URN:	10.1016/j.materresbull.2023.112276

Katalog-ID:	ELV009619895

Internformat


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245	1	0	\|a Tuning electrical heterogeneity in CaCu
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520			\|a Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model.
650		4	\|a CCTO ceramics
650		4	\|a Dielectric properties
650		4	\|a Nonlinear characteristics
650		4	\|a Electrical heterogeneity
650		4	\|a Nano ZnO
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700	1		\|a Liu, Zhiyong \|e verfasserin \|4 aut
700	1		\|a Xie, Bing \|e verfasserin \|4 aut
700	1		\|a Zhao, Yingying \|e verfasserin \|4 aut
700	1		\|a Guo, Kun \|e verfasserin \|0 (orcid)0000-0001-9805-8152 \|4 aut
700	1		\|a Zhang, Lixue \|e verfasserin \|4 aut
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publishDate	2023
allfields	10.1016/j.materresbull.2023.112276 doi (DE-627)ELV009619895 (ELSEVIER)S0025-5408(23)00131-9 DE-627 ger DE-627 rda eng 600 670 VZ 51.00 bkl Mao, Pu verfasserin (orcid)0000-0002-0788-9397 aut Tuning electrical heterogeneity in CaCu 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model. CCTO ceramics Dielectric properties Nonlinear characteristics Electrical heterogeneity Nano ZnO Zeng, Congbin verfasserin aut Guo, Yongguang verfasserin aut Lu, Gang verfasserin aut Yan, Qingsong verfasserin aut Liu, Zhiyong verfasserin aut Xie, Bing verfasserin aut Zhao, Yingying verfasserin aut Guo, Kun verfasserin (orcid)0000-0001-9805-8152 aut Zhang, Lixue verfasserin aut Enthalten in Materials research bulletin New York, NY [u.a.] : Elsevier, 1966 164 Online-Ressource (DE-627)302719466 (DE-600)1491970-9 (DE-576)094422036 nnns volume:164 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 Werkstoffkunde: Allgemeines VZ AR 164
spelling	10.1016/j.materresbull.2023.112276 doi (DE-627)ELV009619895 (ELSEVIER)S0025-5408(23)00131-9 DE-627 ger DE-627 rda eng 600 670 VZ 51.00 bkl Mao, Pu verfasserin (orcid)0000-0002-0788-9397 aut Tuning electrical heterogeneity in CaCu 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model. CCTO ceramics Dielectric properties Nonlinear characteristics Electrical heterogeneity Nano ZnO Zeng, Congbin verfasserin aut Guo, Yongguang verfasserin aut Lu, Gang verfasserin aut Yan, Qingsong verfasserin aut Liu, Zhiyong verfasserin aut Xie, Bing verfasserin aut Zhao, Yingying verfasserin aut Guo, Kun verfasserin (orcid)0000-0001-9805-8152 aut Zhang, Lixue verfasserin aut Enthalten in Materials research bulletin New York, NY [u.a.] : Elsevier, 1966 164 Online-Ressource (DE-627)302719466 (DE-600)1491970-9 (DE-576)094422036 nnns volume:164 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 Werkstoffkunde: Allgemeines VZ AR 164
allfields_unstemmed	10.1016/j.materresbull.2023.112276 doi (DE-627)ELV009619895 (ELSEVIER)S0025-5408(23)00131-9 DE-627 ger DE-627 rda eng 600 670 VZ 51.00 bkl Mao, Pu verfasserin (orcid)0000-0002-0788-9397 aut Tuning electrical heterogeneity in CaCu 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model. CCTO ceramics Dielectric properties Nonlinear characteristics Electrical heterogeneity Nano ZnO Zeng, Congbin verfasserin aut Guo, Yongguang verfasserin aut Lu, Gang verfasserin aut Yan, Qingsong verfasserin aut Liu, Zhiyong verfasserin aut Xie, Bing verfasserin aut Zhao, Yingying verfasserin aut Guo, Kun verfasserin (orcid)0000-0001-9805-8152 aut Zhang, Lixue verfasserin aut Enthalten in Materials research bulletin New York, NY [u.a.] : Elsevier, 1966 164 Online-Ressource (DE-627)302719466 (DE-600)1491970-9 (DE-576)094422036 nnns volume:164 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 Werkstoffkunde: Allgemeines VZ AR 164
allfieldsGer	10.1016/j.materresbull.2023.112276 doi (DE-627)ELV009619895 (ELSEVIER)S0025-5408(23)00131-9 DE-627 ger DE-627 rda eng 600 670 VZ 51.00 bkl Mao, Pu verfasserin (orcid)0000-0002-0788-9397 aut Tuning electrical heterogeneity in CaCu 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model. CCTO ceramics Dielectric properties Nonlinear characteristics Electrical heterogeneity Nano ZnO Zeng, Congbin verfasserin aut Guo, Yongguang verfasserin aut Lu, Gang verfasserin aut Yan, Qingsong verfasserin aut Liu, Zhiyong verfasserin aut Xie, Bing verfasserin aut Zhao, Yingying verfasserin aut Guo, Kun verfasserin (orcid)0000-0001-9805-8152 aut Zhang, Lixue verfasserin aut Enthalten in Materials research bulletin New York, NY [u.a.] : Elsevier, 1966 164 Online-Ressource (DE-627)302719466 (DE-600)1491970-9 (DE-576)094422036 nnns volume:164 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 Werkstoffkunde: Allgemeines VZ AR 164
allfieldsSound	10.1016/j.materresbull.2023.112276 doi (DE-627)ELV009619895 (ELSEVIER)S0025-5408(23)00131-9 DE-627 ger DE-627 rda eng 600 670 VZ 51.00 bkl Mao, Pu verfasserin (orcid)0000-0002-0788-9397 aut Tuning electrical heterogeneity in CaCu 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model. CCTO ceramics Dielectric properties Nonlinear characteristics Electrical heterogeneity Nano ZnO Zeng, Congbin verfasserin aut Guo, Yongguang verfasserin aut Lu, Gang verfasserin aut Yan, Qingsong verfasserin aut Liu, Zhiyong verfasserin aut Xie, Bing verfasserin aut Zhao, Yingying verfasserin aut Guo, Kun verfasserin (orcid)0000-0001-9805-8152 aut Zhang, Lixue verfasserin aut Enthalten in Materials research bulletin New York, NY [u.a.] : Elsevier, 1966 164 Online-Ressource (DE-627)302719466 (DE-600)1491970-9 (DE-576)094422036 nnns volume:164 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 51.00 Werkstoffkunde: Allgemeines VZ AR 164
language	English
source	Enthalten in Materials research bulletin 164 volume:164
sourceStr	Enthalten in Materials research bulletin 164 volume:164
format_phy_str_mv	Article
bklname	Werkstoffkunde: Allgemeines
institution	findex.gbv.de
topic_facet	CCTO ceramics Dielectric properties Nonlinear characteristics Electrical heterogeneity Nano ZnO
dewey-raw	600
isfreeaccess_bool	false
container_title	Materials research bulletin
authorswithroles_txt_mv	Mao, Pu @@aut@@ Zeng, Congbin @@aut@@ Guo, Yongguang @@aut@@ Lu, Gang @@aut@@ Yan, Qingsong @@aut@@ Liu, Zhiyong @@aut@@ Xie, Bing @@aut@@ Zhao, Yingying @@aut@@ Guo, Kun @@aut@@ Zhang, Lixue @@aut@@
publishDateDaySort_date	2023-01-01T00:00:00Z
hierarchy_top_id	302719466
dewey-sort	3600
id	ELV009619895
language_de	englisch
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author	Mao, Pu
spellingShingle	Mao, Pu ddc 600 bkl 51.00 misc CCTO ceramics misc Dielectric properties misc Nonlinear characteristics misc Electrical heterogeneity misc Nano ZnO Tuning electrical heterogeneity in CaCu
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topic_title	600 670 VZ 51.00 bkl Tuning electrical heterogeneity in CaCu CCTO ceramics Dielectric properties Nonlinear characteristics Electrical heterogeneity Nano ZnO
topic	ddc 600 bkl 51.00 misc CCTO ceramics misc Dielectric properties misc Nonlinear characteristics misc Electrical heterogeneity misc Nano ZnO
topic_unstemmed	ddc 600 bkl 51.00 misc CCTO ceramics misc Dielectric properties misc Nonlinear characteristics misc Electrical heterogeneity misc Nano ZnO
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title	Tuning electrical heterogeneity in CaCu
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title_full	Tuning electrical heterogeneity in CaCu
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title_sort	tuning electrical heterogeneity in cacu
title_auth	Tuning electrical heterogeneity in CaCu
abstract	Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model.
abstractGer	Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model.
abstract_unstemmed	Tuning the electrical heterogeneity of CaCu3Ti4O12 (CCTO) ceramic is extremely important to improve its properties. In this work, the CCTO ceramics with enhanced dielectric and nonlinear properties were obtained by the introduction of nano ZnO based on the electrical heterogeneity modulation strategy. As a result, all the CCTO-ZnO samples show the colossal dielectric constant of 104–105 at room temperature. Meanwhile, the dielectric constant of CCTO-ZnO samples exhibits better stability in a wide frequency range from 101 Hz to 105 Hz and over a temperature scope of 30–210 °C. Most importantly, the x = 0.04 sample presents a relatively lower room-temperature dielectric loss of about 0.07 at 103 Hz. Furthermore, the breakdown field strength accompanied by the nonlinear coefficient of CCTO-ZnO ceramics is also improved. The enhancement of dielectric and nonlinear behaviors in these ceramics is mainly ascribed to the tunable electrical heterogeneity as per the internal barrier layer capacitor (IBLC) model.
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title_short	Tuning electrical heterogeneity in CaCu
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author2	Zeng, Congbin Guo, Yongguang Lu, Gang Yan, Qingsong Liu, Zhiyong Xie, Bing Zhao, Yingying Guo, Kun Zhang, Lixue
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up_date	2024-07-06T23:47:01.021Z
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