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Harmonic magneto-dielectric study in doped-, double-, and layered-perovskites
Harmonic magneto-dielectricity studied for the perovskite systems—Pb0.98Gd0.02(Mg1/3Nb2/3)0.995O3 (PGMN), La0.95Ca0.05CoO3 (LCCO), La2NiMnO6 (LNMO), and Ca3Mn2O7 (CMO), precisely characterizes intricately polarized phases. In magnetically co-doped PGMN, the first-harmonic signal ( χ 2 ′ ) manifests...
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Published in: | Journal of applied physics 2020-04, Vol.127 (15) |
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description | Harmonic magneto-dielectricity studied for the perovskite systems—Pb0.98Gd0.02(Mg1/3Nb2/3)0.995O3 (PGMN), La0.95Ca0.05CoO3 (LCCO), La2NiMnO6 (LNMO), and Ca3Mn2O7 (CMO), precisely characterizes intricately polarized phases. In magnetically co-doped PGMN, the first-harmonic signal
(
χ
2
′
) manifests finite polarization P(H) below 270 K, corroborated by the measured remnant P–E traces. The second harmonic
(
χ
3
′
) reveals the effect of random E-fields, causing electrical vitreousity. In spin-state LCCO, across the 65K-start of intermediate- (IS) to low-spin (LS) transition, harmonic susceptibilities evidence IS/LS-interfacial hyper-polarizations, and ac-/dc- conductivities exhibit mechanism-changeovers. In charge-transfer LNMO, dual magneto-electricity due to Ni2+ ↔ Mn4+ charge-hopping (intrinsic) and Maxwell–Wagner (fictitious) polarizations gets distinguished via
χ
2
′. In hybrid improper ferroelectric (HIF) CMO, while the
χ
2
,
3
′-signals clearly evidence stabilization of the ferroelectric state below 50 K,
χ
3
′ and ɛ* discern the super-paraelectric, coupled-relaxor, and glassy phases, magneto-electrically coexistent with short-range spin-correlations, antiferromagnetic, and weak-ferromagnetic states, respectively. Our results on a variety of perovskites establish harmonics' exclusivity in revealing novel phases and superiority in divulging subtly variant states, either escaping detection or rendered indescript by usual electrical characterizations. |
doi_str_mv | 10.1063/1.5145383 |
format | article |
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(
χ
2
′
) manifests finite polarization P(H) below 270 K, corroborated by the measured remnant P–E traces. The second harmonic
(
χ
3
′
) reveals the effect of random E-fields, causing electrical vitreousity. In spin-state LCCO, across the 65K-start of intermediate- (IS) to low-spin (LS) transition, harmonic susceptibilities evidence IS/LS-interfacial hyper-polarizations, and ac-/dc- conductivities exhibit mechanism-changeovers. In charge-transfer LNMO, dual magneto-electricity due to Ni2+ ↔ Mn4+ charge-hopping (intrinsic) and Maxwell–Wagner (fictitious) polarizations gets distinguished via
χ
2
′. In hybrid improper ferroelectric (HIF) CMO, while the
χ
2
,
3
′-signals clearly evidence stabilization of the ferroelectric state below 50 K,
χ
3
′ and ɛ* discern the super-paraelectric, coupled-relaxor, and glassy phases, magneto-electrically coexistent with short-range spin-correlations, antiferromagnetic, and weak-ferromagnetic states, respectively. Our results on a variety of perovskites establish harmonics' exclusivity in revealing novel phases and superiority in divulging subtly variant states, either escaping detection or rendered indescript by usual electrical characterizations.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.5145383</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Antiferromagnetism ; Applied physics ; Charge transfer ; Chi-square test ; Ferroelectric materials ; Ferroelectricity ; Ferromagnetism ; Manganese ; Perovskites ; Phases ; Relaxors</subject><ispartof>Journal of applied physics, 2020-04, Vol.127 (15)</ispartof><rights>Author(s)</rights><rights>2020 Author(s). Published under license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c327t-7bc84dd70f975f668ea83f847de30efabc2e4cf882ec4c8302780f35cfa7c0fb3</citedby><cites>FETCH-LOGICAL-c327t-7bc84dd70f975f668ea83f847de30efabc2e4cf882ec4c8302780f35cfa7c0fb3</cites><orcidid>0000-0002-7345-2038</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Sahlot, Pooja</creatorcontrib><creatorcontrib>Pandey, Suchita</creatorcontrib><creatorcontrib>Pandey, Adityanarayan</creatorcontrib><creatorcontrib>Awasthi, A. M.</creatorcontrib><title>Harmonic magneto-dielectric study in doped-, double-, and layered-perovskites</title><title>Journal of applied physics</title><description>Harmonic magneto-dielectricity studied for the perovskite systems—Pb0.98Gd0.02(Mg1/3Nb2/3)0.995O3 (PGMN), La0.95Ca0.05CoO3 (LCCO), La2NiMnO6 (LNMO), and Ca3Mn2O7 (CMO), precisely characterizes intricately polarized phases. In magnetically co-doped PGMN, the first-harmonic signal
(
χ
2
′
) manifests finite polarization P(H) below 270 K, corroborated by the measured remnant P–E traces. The second harmonic
(
χ
3
′
) reveals the effect of random E-fields, causing electrical vitreousity. In spin-state LCCO, across the 65K-start of intermediate- (IS) to low-spin (LS) transition, harmonic susceptibilities evidence IS/LS-interfacial hyper-polarizations, and ac-/dc- conductivities exhibit mechanism-changeovers. In charge-transfer LNMO, dual magneto-electricity due to Ni2+ ↔ Mn4+ charge-hopping (intrinsic) and Maxwell–Wagner (fictitious) polarizations gets distinguished via
χ
2
′. In hybrid improper ferroelectric (HIF) CMO, while the
χ
2
,
3
′-signals clearly evidence stabilization of the ferroelectric state below 50 K,
χ
3
′ and ɛ* discern the super-paraelectric, coupled-relaxor, and glassy phases, magneto-electrically coexistent with short-range spin-correlations, antiferromagnetic, and weak-ferromagnetic states, respectively. Our results on a variety of perovskites establish harmonics' exclusivity in revealing novel phases and superiority in divulging subtly variant states, either escaping detection or rendered indescript by usual electrical characterizations.</description><subject>Antiferromagnetism</subject><subject>Applied physics</subject><subject>Charge transfer</subject><subject>Chi-square test</subject><subject>Ferroelectric materials</subject><subject>Ferroelectricity</subject><subject>Ferromagnetism</subject><subject>Manganese</subject><subject>Perovskites</subject><subject>Phases</subject><subject>Relaxors</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNqd0MFKAzEQBuAgCtbqwTdY8KSYmmx2m-xRSrVCxYueQzaZSOp2sybZQt_eSAvePf3D8DEDP0LXlMwombMHOqtpVTPBTtCEEtFgXtfkFE0IKSkWDW_O0UWMG0IoFayZoNeVClvfO11s1WcPyWPjoAOdQl7FNJp94frC-AEMvs85th3kQfWm6NQeQl4PEPwufrkE8RKdWdVFuDrmFH08Ld8XK7x-e35ZPK6xZiVPmLdaVMZwYhte2_lcgBLMioobYASsanUJlbZClKArLRgpuSCW1doqrolt2RTdHO4OwX-PEJPc-DH0-aUsWVNSyjlnWd0elA4-xgBWDsFtVdhLSuRvW5LKY1vZ3h1s1C6p5Hz_P7zz4Q_KwVj2AyFceJM</recordid><startdate>20200421</startdate><enddate>20200421</enddate><creator>Sahlot, Pooja</creator><creator>Pandey, Suchita</creator><creator>Pandey, Adityanarayan</creator><creator>Awasthi, A. M.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-7345-2038</orcidid></search><sort><creationdate>20200421</creationdate><title>Harmonic magneto-dielectric study in doped-, double-, and layered-perovskites</title><author>Sahlot, Pooja ; Pandey, Suchita ; Pandey, Adityanarayan ; Awasthi, A. M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c327t-7bc84dd70f975f668ea83f847de30efabc2e4cf882ec4c8302780f35cfa7c0fb3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Antiferromagnetism</topic><topic>Applied physics</topic><topic>Charge transfer</topic><topic>Chi-square test</topic><topic>Ferroelectric materials</topic><topic>Ferroelectricity</topic><topic>Ferromagnetism</topic><topic>Manganese</topic><topic>Perovskites</topic><topic>Phases</topic><topic>Relaxors</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sahlot, Pooja</creatorcontrib><creatorcontrib>Pandey, Suchita</creatorcontrib><creatorcontrib>Pandey, Adityanarayan</creatorcontrib><creatorcontrib>Awasthi, A. M.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sahlot, Pooja</au><au>Pandey, Suchita</au><au>Pandey, Adityanarayan</au><au>Awasthi, A. M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Harmonic magneto-dielectric study in doped-, double-, and layered-perovskites</atitle><jtitle>Journal of applied physics</jtitle><date>2020-04-21</date><risdate>2020</risdate><volume>127</volume><issue>15</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>Harmonic magneto-dielectricity studied for the perovskite systems—Pb0.98Gd0.02(Mg1/3Nb2/3)0.995O3 (PGMN), La0.95Ca0.05CoO3 (LCCO), La2NiMnO6 (LNMO), and Ca3Mn2O7 (CMO), precisely characterizes intricately polarized phases. In magnetically co-doped PGMN, the first-harmonic signal
(
χ
2
′
) manifests finite polarization P(H) below 270 K, corroborated by the measured remnant P–E traces. The second harmonic
(
χ
3
′
) reveals the effect of random E-fields, causing electrical vitreousity. In spin-state LCCO, across the 65K-start of intermediate- (IS) to low-spin (LS) transition, harmonic susceptibilities evidence IS/LS-interfacial hyper-polarizations, and ac-/dc- conductivities exhibit mechanism-changeovers. In charge-transfer LNMO, dual magneto-electricity due to Ni2+ ↔ Mn4+ charge-hopping (intrinsic) and Maxwell–Wagner (fictitious) polarizations gets distinguished via
χ
2
′. In hybrid improper ferroelectric (HIF) CMO, while the
χ
2
,
3
′-signals clearly evidence stabilization of the ferroelectric state below 50 K,
χ
3
′ and ɛ* discern the super-paraelectric, coupled-relaxor, and glassy phases, magneto-electrically coexistent with short-range spin-correlations, antiferromagnetic, and weak-ferromagnetic states, respectively. Our results on a variety of perovskites establish harmonics' exclusivity in revealing novel phases and superiority in divulging subtly variant states, either escaping detection or rendered indescript by usual electrical characterizations.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.5145383</doi><tpages>13</tpages><orcidid>https://orcid.org/0000-0002-7345-2038</orcidid></addata></record> |
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source | American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list) |
subjects | Antiferromagnetism Applied physics Charge transfer Chi-square test Ferroelectric materials Ferroelectricity Ferromagnetism Manganese Perovskites Phases Relaxors |
title | Harmonic magneto-dielectric study in doped-, double-, and layered-perovskites |
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