Effect of CoFe

Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate compos...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Pal, Munendra [verfasserIn] Srinivas, Adiraj [verfasserIn] Asthana, Saket [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2023

Schlagwörter:	Magnetoelectric particulate composite Domain reversal Scaling behaviour Dynamic hysteresis Leakage current

Übergeordnetes Werk:	Enthalten in: Physica / B - Amsterdam : Elsevier, 1988, 666
Übergeordnetes Werk:	volume:666

DOI / URN:	10.1016/j.physb.2023.415127

Katalog-ID:	ELV062114689

Internformat


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520			\|a Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal.
650		4	\|a Magnetoelectric particulate composite
650		4	\|a Domain reversal
650		4	\|a Scaling behaviour
650		4	\|a Dynamic hysteresis
650		4	\|a Leakage current
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700	1		\|a Asthana, Saket \|e verfasserin \|4 aut
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Indexfelder

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bklnumber	33.60 51.00
publishDate	2023
allfields	10.1016/j.physb.2023.415127 doi (DE-627)ELV062114689 (ELSEVIER)S0921-4526(23)00494-5 DE-627 ger DE-627 rda eng 530 VZ 33.60 bkl 51.00 bkl Pal, Munendra verfasserin aut Effect of CoFe 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal. Magnetoelectric particulate composite Domain reversal Scaling behaviour Dynamic hysteresis Leakage current Srinivas, Adiraj verfasserin aut Asthana, Saket verfasserin aut Enthalten in Physica / B Amsterdam : Elsevier, 1988 666 Online-Ressource (DE-627)266015093 (DE-600)1466579-7 (DE-576)074959840 1873-2135 nnns volume:666 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_101 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 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 666
spelling	10.1016/j.physb.2023.415127 doi (DE-627)ELV062114689 (ELSEVIER)S0921-4526(23)00494-5 DE-627 ger DE-627 rda eng 530 VZ 33.60 bkl 51.00 bkl Pal, Munendra verfasserin aut Effect of CoFe 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal. Magnetoelectric particulate composite Domain reversal Scaling behaviour Dynamic hysteresis Leakage current Srinivas, Adiraj verfasserin aut Asthana, Saket verfasserin aut Enthalten in Physica / B Amsterdam : Elsevier, 1988 666 Online-Ressource (DE-627)266015093 (DE-600)1466579-7 (DE-576)074959840 1873-2135 nnns volume:666 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_101 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 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 666
allfields_unstemmed	10.1016/j.physb.2023.415127 doi (DE-627)ELV062114689 (ELSEVIER)S0921-4526(23)00494-5 DE-627 ger DE-627 rda eng 530 VZ 33.60 bkl 51.00 bkl Pal, Munendra verfasserin aut Effect of CoFe 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal. Magnetoelectric particulate composite Domain reversal Scaling behaviour Dynamic hysteresis Leakage current Srinivas, Adiraj verfasserin aut Asthana, Saket verfasserin aut Enthalten in Physica / B Amsterdam : Elsevier, 1988 666 Online-Ressource (DE-627)266015093 (DE-600)1466579-7 (DE-576)074959840 1873-2135 nnns volume:666 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_101 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 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 666
allfieldsGer	10.1016/j.physb.2023.415127 doi (DE-627)ELV062114689 (ELSEVIER)S0921-4526(23)00494-5 DE-627 ger DE-627 rda eng 530 VZ 33.60 bkl 51.00 bkl Pal, Munendra verfasserin aut Effect of CoFe 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal. Magnetoelectric particulate composite Domain reversal Scaling behaviour Dynamic hysteresis Leakage current Srinivas, Adiraj verfasserin aut Asthana, Saket verfasserin aut Enthalten in Physica / B Amsterdam : Elsevier, 1988 666 Online-Ressource (DE-627)266015093 (DE-600)1466579-7 (DE-576)074959840 1873-2135 nnns volume:666 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_101 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 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 666
allfieldsSound	10.1016/j.physb.2023.415127 doi (DE-627)ELV062114689 (ELSEVIER)S0921-4526(23)00494-5 DE-627 ger DE-627 rda eng 530 VZ 33.60 bkl 51.00 bkl Pal, Munendra verfasserin aut Effect of CoFe 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal. Magnetoelectric particulate composite Domain reversal Scaling behaviour Dynamic hysteresis Leakage current Srinivas, Adiraj verfasserin aut Asthana, Saket verfasserin aut Enthalten in Physica / B Amsterdam : Elsevier, 1988 666 Online-Ressource (DE-627)266015093 (DE-600)1466579-7 (DE-576)074959840 1873-2135 nnns volume:666 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_101 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 33.60 Kondensierte Materie: Allgemeines VZ 51.00 Werkstoffkunde: Allgemeines VZ AR 666
language	English
source	Enthalten in Physica / B 666 volume:666
sourceStr	Enthalten in Physica / B 666 volume:666
format_phy_str_mv	Article
bklname	Kondensierte Materie: Allgemeines Werkstoffkunde: Allgemeines
institution	findex.gbv.de
topic_facet	Magnetoelectric particulate composite Domain reversal Scaling behaviour Dynamic hysteresis Leakage current
dewey-raw	530
isfreeaccess_bool	false
container_title	Physica / B
authorswithroles_txt_mv	Pal, Munendra @@aut@@ Srinivas, Adiraj @@aut@@ Asthana, Saket @@aut@@
publishDateDaySort_date	2023-01-01T00:00:00Z
hierarchy_top_id	266015093
dewey-sort	3530
id	ELV062114689
language_de	englisch
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author	Pal, Munendra
spellingShingle	Pal, Munendra ddc 530 bkl 33.60 bkl 51.00 misc Magnetoelectric particulate composite misc Domain reversal misc Scaling behaviour misc Dynamic hysteresis misc Leakage current Effect of CoFe
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topic_title	530 VZ 33.60 bkl 51.00 bkl Effect of CoFe Magnetoelectric particulate composite Domain reversal Scaling behaviour Dynamic hysteresis Leakage current
topic	ddc 530 bkl 33.60 bkl 51.00 misc Magnetoelectric particulate composite misc Domain reversal misc Scaling behaviour misc Dynamic hysteresis misc Leakage current
topic_unstemmed	ddc 530 bkl 33.60 bkl 51.00 misc Magnetoelectric particulate composite misc Domain reversal misc Scaling behaviour misc Dynamic hysteresis misc Leakage current
topic_browse	ddc 530 bkl 33.60 bkl 51.00 misc Magnetoelectric particulate composite misc Domain reversal misc Scaling behaviour misc Dynamic hysteresis misc Leakage current
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title	Effect of CoFe
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title_full	Effect of CoFe
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author_browse	Pal, Munendra Srinivas, Adiraj Asthana, Saket
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title_sort	effect of cofe
title_auth	Effect of CoFe
abstract	Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal.
abstractGer	Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal.
abstract_unstemmed	Many technological applications of ferroelectric materials are fundamentally connected to domain reversal under the electric field. Here the polarization reversible mechanism has been studied in (1-x)(0.94Na0·5Bi0·5TiO3-0.06BaTiO3)–x(CoFe2O4) (NBBT-CFO) (x = 0, 15, 25 and 35 mol%) particulate composites through the electric field and frequency-dependent scaling behavior of their hysteresis loop. Along with this, the role of the CFO on the polarization reversal processes of NBBT has been investigated systematically. Three-stage behaviour has been observed in the polarization reversal for all the systems. The observed scaling parameter β value for the composites is found to be less than parent NBBT, which has been discussed based on the pinning effect that arises due to the CFO phase. The induced pinning effect in the composites is due to the high leakage current which is confirmed by the leakage current density (J) measurement. The scaling relation of loop area <A> versus E 0 and ƒ for the composites is followed by the power law < A > ∝ f − 0.265 E 0 1.320 in the saturated region. The present findings may be useful in technological applications related to polarization reversal.
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title_short	Effect of CoFe
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author2	Srinivas, Adiraj Asthana, Saket
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up_date	2024-07-06T18:25:08.569Z
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score	7.3982143

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