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Enhancement of electrical and magnetic properties in acceptor-doped BaTiO3 ferroelectric ceramics
BaTi 1−x Mn x O 3 (x = 0.00, 0.25, 0.50, 0.75 mol%) (BTMO) ceramics were synthesized through sol–gel combustion method. The structural studies suggested that Mn-doped BaTiO 3 (BTO) ceramics exhibit a tetragonal structure with P 4 mm space group via Rietveld refinement analysis. Also, the phonon mode...
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Published in: | Journal of materials science. Materials in electronics 2019-02, Vol.30 (3), p.2953-2965 |
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creator | Madhan, K. Jagadeeshwaran, C. Murugaraj, R. |
description | BaTi
1−x
Mn
x
O
3
(x = 0.00, 0.25, 0.50, 0.75 mol%) (BTMO) ceramics were synthesized through sol–gel combustion method. The structural studies suggested that Mn-doped BaTiO
3
(BTO) ceramics exhibit a tetragonal structure with
P
4
mm
space group via Rietveld refinement analysis. Also, the phonon mode at 308 cm
−1
through Raman spectral analysis confirms the local structure of tetragonal symmetries. The redshift observed in UV-absorption spectra indicates a decrease of optical band gap from 3.13 to 2.71 eV with increasing Mn
2+
doping. The observed decrease in the intensity of PL emission spectra was due to an increase of Mn
2+
concentration. This indicates that a decrease in oxygen vacancies and a reduction in the number of electrons attributed to the Burstein–Moss shift. The carrier hopping process between Mn
2+
and Mn
3+
is responsible for dielectric as well as magnetization behavior. The ferroelectric double hysteresis loops are related to a ferroelectric and anti-ferroelectric order and it increases with the increase of Mn ion concentration in BTO. Through P–E measurements, the value of remnant electric polarization and coercive field found to be increased with Mn concentration in BTO samples. For BTO sample, two EPR signals with g = 1.969 and g = 2.000 singlets can be assigned with ionized Ba and Ti-vacancy defects. In addition, the EPR signal for BTMO shows a good correlation with Ti vacancies as compensating for lattice defects. Further, the Mn doping induced a weak ferromagnetic to ferromagnetic state due to free carrier concentrations. |
doi_str_mv | 10.1007/s10854-018-00573-6 |
format | article |
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1−x
Mn
x
O
3
(x = 0.00, 0.25, 0.50, 0.75 mol%) (BTMO) ceramics were synthesized through sol–gel combustion method. The structural studies suggested that Mn-doped BaTiO
3
(BTO) ceramics exhibit a tetragonal structure with
P
4
mm
space group via Rietveld refinement analysis. Also, the phonon mode at 308 cm
−1
through Raman spectral analysis confirms the local structure of tetragonal symmetries. The redshift observed in UV-absorption spectra indicates a decrease of optical band gap from 3.13 to 2.71 eV with increasing Mn
2+
doping. The observed decrease in the intensity of PL emission spectra was due to an increase of Mn
2+
concentration. This indicates that a decrease in oxygen vacancies and a reduction in the number of electrons attributed to the Burstein–Moss shift. The carrier hopping process between Mn
2+
and Mn
3+
is responsible for dielectric as well as magnetization behavior. The ferroelectric double hysteresis loops are related to a ferroelectric and anti-ferroelectric order and it increases with the increase of Mn ion concentration in BTO. Through P–E measurements, the value of remnant electric polarization and coercive field found to be increased with Mn concentration in BTO samples. For BTO sample, two EPR signals with g = 1.969 and g = 2.000 singlets can be assigned with ionized Ba and Ti-vacancy defects. In addition, the EPR signal for BTMO shows a good correlation with Ti vacancies as compensating for lattice defects. Further, the Mn doping induced a weak ferromagnetic to ferromagnetic state due to free carrier concentrations.</description><identifier>ISSN: 0957-4522</identifier><identifier>EISSN: 1573-482X</identifier><identifier>DOI: 10.1007/s10854-018-00573-6</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Absorption spectra ; Acids ; Antiferroelectricity ; Barium titanates ; Carrier density ; Ceramics ; Characterization and Evaluation of Materials ; Chemistry and Materials Science ; Coercivity ; Crystal defects ; Doping ; Electric polarization ; Emission spectra ; Ferroelectric materials ; Ferromagnetism ; Grain size ; Hysteresis loops ; Ion concentration ; Lattice vacancies ; Magnetic properties ; Materials Science ; Nitrates ; Optical and Electronic Materials ; Phase transitions ; Red shift ; Sol-gel processes</subject><ispartof>Journal of materials science. Materials in electronics, 2019-02, Vol.30 (3), p.2953-2965</ispartof><rights>Springer Science+Business Media, LLC, part of Springer Nature 2019</rights><rights>Journal of Materials Science: Materials in Electronics is a copyright of Springer, (2019). All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c249t-8372a2df7e835673867ba4e67616fc63c6b5cdbd2389ab56a2858f43f4766abd3</citedby><cites>FETCH-LOGICAL-c249t-8372a2df7e835673867ba4e67616fc63c6b5cdbd2389ab56a2858f43f4766abd3</cites><orcidid>0000-0002-8118-5478</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>Madhan, K.</creatorcontrib><creatorcontrib>Jagadeeshwaran, C.</creatorcontrib><creatorcontrib>Murugaraj, R.</creatorcontrib><title>Enhancement of electrical and magnetic properties in acceptor-doped BaTiO3 ferroelectric ceramics</title><title>Journal of materials science. Materials in electronics</title><addtitle>J Mater Sci: Mater Electron</addtitle><description>BaTi
1−x
Mn
x
O
3
(x = 0.00, 0.25, 0.50, 0.75 mol%) (BTMO) ceramics were synthesized through sol–gel combustion method. The structural studies suggested that Mn-doped BaTiO
3
(BTO) ceramics exhibit a tetragonal structure with
P
4
mm
space group via Rietveld refinement analysis. Also, the phonon mode at 308 cm
−1
through Raman spectral analysis confirms the local structure of tetragonal symmetries. The redshift observed in UV-absorption spectra indicates a decrease of optical band gap from 3.13 to 2.71 eV with increasing Mn
2+
doping. The observed decrease in the intensity of PL emission spectra was due to an increase of Mn
2+
concentration. This indicates that a decrease in oxygen vacancies and a reduction in the number of electrons attributed to the Burstein–Moss shift. The carrier hopping process between Mn
2+
and Mn
3+
is responsible for dielectric as well as magnetization behavior. The ferroelectric double hysteresis loops are related to a ferroelectric and anti-ferroelectric order and it increases with the increase of Mn ion concentration in BTO. Through P–E measurements, the value of remnant electric polarization and coercive field found to be increased with Mn concentration in BTO samples. For BTO sample, two EPR signals with g = 1.969 and g = 2.000 singlets can be assigned with ionized Ba and Ti-vacancy defects. In addition, the EPR signal for BTMO shows a good correlation with Ti vacancies as compensating for lattice defects. Further, the Mn doping induced a weak ferromagnetic to ferromagnetic state due to free carrier concentrations.</description><subject>Absorption spectra</subject><subject>Acids</subject><subject>Antiferroelectricity</subject><subject>Barium titanates</subject><subject>Carrier density</subject><subject>Ceramics</subject><subject>Characterization and Evaluation of Materials</subject><subject>Chemistry and Materials Science</subject><subject>Coercivity</subject><subject>Crystal defects</subject><subject>Doping</subject><subject>Electric polarization</subject><subject>Emission spectra</subject><subject>Ferroelectric materials</subject><subject>Ferromagnetism</subject><subject>Grain size</subject><subject>Hysteresis loops</subject><subject>Ion concentration</subject><subject>Lattice vacancies</subject><subject>Magnetic properties</subject><subject>Materials Science</subject><subject>Nitrates</subject><subject>Optical and Electronic Materials</subject><subject>Phase transitions</subject><subject>Red shift</subject><subject>Sol-gel processes</subject><issn>0957-4522</issn><issn>1573-482X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp9kEtLAzEUhYMoWKt_wFXAdTTvpEst9QGFbiq4C5nMTZ3SydRkuvDfO3UUd67u5XLOuYcPoWtGbxml5q4wapUklFlCqTKC6BM0YcdFWv52iiZ0pgyRivNzdFHKllKqpbAT5Bfp3acALaQedxHDDkKfm-B32Kcat36ToG8C3uduD7lvoOAmYR8C7Psuk3q41vjBr5uVwBFy7n4DcIDs2yaUS3QW_a7A1c-cotfHxXr-TJarp5f5_ZIELmc9scJwz-towAqljbDaVF6CNprpGLQIulKhrmou7MxXSntulY1SRGm09lUtpuhmzB2qfhyg9G7bHXIaXjrONNeGMykGFR9VIXelZIhun5vW50_HqDuidCNKN6B03yidHkxiNJVBnDaQ_6L_cX0Be253aw</recordid><startdate>20190201</startdate><enddate>20190201</enddate><creator>Madhan, K.</creator><creator>Jagadeeshwaran, C.</creator><creator>Murugaraj, R.</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>F28</scope><scope>FR3</scope><scope>HCIFZ</scope><scope>JG9</scope><scope>KB.</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PDBOC</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>S0W</scope><orcidid>https://orcid.org/0000-0002-8118-5478</orcidid></search><sort><creationdate>20190201</creationdate><title>Enhancement of electrical and magnetic properties in acceptor-doped BaTiO3 ferroelectric ceramics</title><author>Madhan, K. ; Jagadeeshwaran, C. ; Murugaraj, R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c249t-8372a2df7e835673867ba4e67616fc63c6b5cdbd2389ab56a2858f43f4766abd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Absorption spectra</topic><topic>Acids</topic><topic>Antiferroelectricity</topic><topic>Barium titanates</topic><topic>Carrier density</topic><topic>Ceramics</topic><topic>Characterization and Evaluation of Materials</topic><topic>Chemistry and Materials Science</topic><topic>Coercivity</topic><topic>Crystal defects</topic><topic>Doping</topic><topic>Electric polarization</topic><topic>Emission spectra</topic><topic>Ferroelectric materials</topic><topic>Ferromagnetism</topic><topic>Grain size</topic><topic>Hysteresis loops</topic><topic>Ion concentration</topic><topic>Lattice vacancies</topic><topic>Magnetic properties</topic><topic>Materials Science</topic><topic>Nitrates</topic><topic>Optical and Electronic Materials</topic><topic>Phase transitions</topic><topic>Red shift</topic><topic>Sol-gel processes</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Madhan, K.</creatorcontrib><creatorcontrib>Jagadeeshwaran, C.</creatorcontrib><creatorcontrib>Murugaraj, R.</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>SciTech Premium Collection (Proquest) (PQ_SDU_P3)</collection><collection>Materials Research Database</collection><collection>https://resources.nclive.org/materials</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>ProQuest advanced technologies & aerospace journals</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Materials science collection</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>DELNET Engineering & Technology Collection</collection><jtitle>Journal of materials science. Materials in electronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Madhan, K.</au><au>Jagadeeshwaran, C.</au><au>Murugaraj, R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Enhancement of electrical and magnetic properties in acceptor-doped BaTiO3 ferroelectric ceramics</atitle><jtitle>Journal of materials science. Materials in electronics</jtitle><stitle>J Mater Sci: Mater Electron</stitle><date>2019-02-01</date><risdate>2019</risdate><volume>30</volume><issue>3</issue><spage>2953</spage><epage>2965</epage><pages>2953-2965</pages><issn>0957-4522</issn><eissn>1573-482X</eissn><abstract>BaTi
1−x
Mn
x
O
3
(x = 0.00, 0.25, 0.50, 0.75 mol%) (BTMO) ceramics were synthesized through sol–gel combustion method. The structural studies suggested that Mn-doped BaTiO
3
(BTO) ceramics exhibit a tetragonal structure with
P
4
mm
space group via Rietveld refinement analysis. Also, the phonon mode at 308 cm
−1
through Raman spectral analysis confirms the local structure of tetragonal symmetries. The redshift observed in UV-absorption spectra indicates a decrease of optical band gap from 3.13 to 2.71 eV with increasing Mn
2+
doping. The observed decrease in the intensity of PL emission spectra was due to an increase of Mn
2+
concentration. This indicates that a decrease in oxygen vacancies and a reduction in the number of electrons attributed to the Burstein–Moss shift. The carrier hopping process between Mn
2+
and Mn
3+
is responsible for dielectric as well as magnetization behavior. The ferroelectric double hysteresis loops are related to a ferroelectric and anti-ferroelectric order and it increases with the increase of Mn ion concentration in BTO. Through P–E measurements, the value of remnant electric polarization and coercive field found to be increased with Mn concentration in BTO samples. For BTO sample, two EPR signals with g = 1.969 and g = 2.000 singlets can be assigned with ionized Ba and Ti-vacancy defects. In addition, the EPR signal for BTMO shows a good correlation with Ti vacancies as compensating for lattice defects. Further, the Mn doping induced a weak ferromagnetic to ferromagnetic state due to free carrier concentrations.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s10854-018-00573-6</doi><tpages>13</tpages><orcidid>https://orcid.org/0000-0002-8118-5478</orcidid></addata></record> |
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subjects | Absorption spectra Acids Antiferroelectricity Barium titanates Carrier density Ceramics Characterization and Evaluation of Materials Chemistry and Materials Science Coercivity Crystal defects Doping Electric polarization Emission spectra Ferroelectric materials Ferromagnetism Grain size Hysteresis loops Ion concentration Lattice vacancies Magnetic properties Materials Science Nitrates Optical and Electronic Materials Phase transitions Red shift Sol-gel processes |
title | Enhancement of electrical and magnetic properties in acceptor-doped BaTiO3 ferroelectric ceramics |
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