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Formation of non-centrosymmetric covalent bonds due to the substitution of cobalt contents in M-type barium hexa-ferrites BaFe(12-x)O19
The evolution of various properties of cobalt-doped M-type barium hexa-ferrites has been investigated in this project. A series of cobalt-doped M-type barium hexa-ferrites having general composition BaCo x Fe (12-x) O 19 with x = 0.2, 0.4, 0.6, 0.8, 1.0, and 1.2 was prepared using powder metallurgy...
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Published in: | Applied physics. A, Materials science & processing Materials science & processing, 2021-09, Vol.127 (9), Article 718 |
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description | The evolution of various properties of cobalt-doped M-type barium hexa-ferrites has been investigated in this project. A series of cobalt-doped M-type barium hexa-ferrites having general composition BaCo
x
Fe
(12-x)
O
19
with x = 0.2, 0.4, 0.6, 0.8, 1.0, and 1.2 was prepared using powder metallurgy route. For the thermal decomposition, prepared powders were heat-treated at 1373 K
o
for 2 h in a muffle furnace. The structural analysis, 3-D structural visualization, functional group analysis, surface morphology, elemental analysis, optical, dielectric, ferromagnetic, and ferroelectric properties of samples were characterized using different characterization techniques. X-ray diffractometer and Fourier transform infrared spectroscopy confirmed the formation of single-phase hexagonal structure of cobalt-doped M-type barium hexa-ferrite. The optical bandgap energy and saturation magnetization of the prepared samples increased with increasing cobalt concentration which made them suitable for light-emitting diodes and laser formation. Their dielectric properties show the insulting nature of the ferrites. Ferro-electric loop exhibits formation of non-centrosymmetric covalent bonds with an increase in the electric coercive field and remanent polarization. The electric polarization in the unit cell of barium hexa-ferrites is based on FeO6 octahedron. The oxygen O6 is located at three crystallographic sites (4f, 2a and 12 k). The iron ion is normally located at the center of the oxygen octahedron. The formation of non-centrosymmetric covalent bonds is due to the shifts off-center of iron ions under the application of external field. The ferroelectric loops are also not properly closed which indicates the magnetoelectric (ME) coupling and improves multiferroicity of the material. |
doi_str_mv | 10.1007/s00339-021-04762-9 |
format | article |
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x
Fe
(12-x)
O
19
with x = 0.2, 0.4, 0.6, 0.8, 1.0, and 1.2 was prepared using powder metallurgy route. For the thermal decomposition, prepared powders were heat-treated at 1373 K
o
for 2 h in a muffle furnace. The structural analysis, 3-D structural visualization, functional group analysis, surface morphology, elemental analysis, optical, dielectric, ferromagnetic, and ferroelectric properties of samples were characterized using different characterization techniques. X-ray diffractometer and Fourier transform infrared spectroscopy confirmed the formation of single-phase hexagonal structure of cobalt-doped M-type barium hexa-ferrite. The optical bandgap energy and saturation magnetization of the prepared samples increased with increasing cobalt concentration which made them suitable for light-emitting diodes and laser formation. Their dielectric properties show the insulting nature of the ferrites. Ferro-electric loop exhibits formation of non-centrosymmetric covalent bonds with an increase in the electric coercive field and remanent polarization. The electric polarization in the unit cell of barium hexa-ferrites is based on FeO6 octahedron. The oxygen O6 is located at three crystallographic sites (4f, 2a and 12 k). The iron ion is normally located at the center of the oxygen octahedron. The formation of non-centrosymmetric covalent bonds is due to the shifts off-center of iron ions under the application of external field. The ferroelectric loops are also not properly closed which indicates the magnetoelectric (ME) coupling and improves multiferroicity of the material.</description><identifier>ISSN: 0947-8396</identifier><identifier>EISSN: 1432-0630</identifier><identifier>DOI: 10.1007/s00339-021-04762-9</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Applied physics ; Barium ; Characterization and Evaluation of Materials ; Chemical bonds ; Cobalt ; Coercivity ; Condensed Matter Physics ; Covalence ; Covalent bonds ; Crystallography ; Dielectric properties ; Electric polarization ; Ferrites ; Ferroelectric materials ; Ferroelectricity ; Ferromagnetism ; Functional groups ; Heat treatment ; Iron ; Light emitting diodes ; Machines ; Magnetic saturation ; Manufacturing ; Materials science ; Morphology ; Muffle furnaces ; Nanotechnology ; Optical and Electronic Materials ; Optical properties ; Physics ; Physics and Astronomy ; Powder metallurgy ; Processes ; Structural analysis ; Surfaces and Interfaces ; Thermal decomposition ; Thin Films ; Unit cell</subject><ispartof>Applied physics. A, Materials science & processing, 2021-09, Vol.127 (9), Article 718</ispartof><rights>The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2021</rights><rights>The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2021.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c270t-313bca09f5287afbcbe2a2b7272ba41f892fa1aea21f4e82c0e109ff453999353</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,27905,27906</link.rule.ids></links><search><creatorcontrib>Sehar, Fatima</creatorcontrib><creatorcontrib>Anjum, Safia</creatorcontrib><creatorcontrib>Mansoor, Anam</creatorcontrib><creatorcontrib>Mustafa, Zeeshan</creatorcontrib><title>Formation of non-centrosymmetric covalent bonds due to the substitution of cobalt contents in M-type barium hexa-ferrites BaFe(12-x)O19</title><title>Applied physics. A, Materials science & processing</title><addtitle>Appl. Phys. A</addtitle><description>The evolution of various properties of cobalt-doped M-type barium hexa-ferrites has been investigated in this project. A series of cobalt-doped M-type barium hexa-ferrites having general composition BaCo
x
Fe
(12-x)
O
19
with x = 0.2, 0.4, 0.6, 0.8, 1.0, and 1.2 was prepared using powder metallurgy route. For the thermal decomposition, prepared powders were heat-treated at 1373 K
o
for 2 h in a muffle furnace. The structural analysis, 3-D structural visualization, functional group analysis, surface morphology, elemental analysis, optical, dielectric, ferromagnetic, and ferroelectric properties of samples were characterized using different characterization techniques. X-ray diffractometer and Fourier transform infrared spectroscopy confirmed the formation of single-phase hexagonal structure of cobalt-doped M-type barium hexa-ferrite. The optical bandgap energy and saturation magnetization of the prepared samples increased with increasing cobalt concentration which made them suitable for light-emitting diodes and laser formation. Their dielectric properties show the insulting nature of the ferrites. Ferro-electric loop exhibits formation of non-centrosymmetric covalent bonds with an increase in the electric coercive field and remanent polarization. The electric polarization in the unit cell of barium hexa-ferrites is based on FeO6 octahedron. The oxygen O6 is located at three crystallographic sites (4f, 2a and 12 k). The iron ion is normally located at the center of the oxygen octahedron. The formation of non-centrosymmetric covalent bonds is due to the shifts off-center of iron ions under the application of external field. The ferroelectric loops are also not properly closed which indicates the magnetoelectric (ME) coupling and improves multiferroicity of the material.</description><subject>Applied physics</subject><subject>Barium</subject><subject>Characterization and Evaluation of Materials</subject><subject>Chemical bonds</subject><subject>Cobalt</subject><subject>Coercivity</subject><subject>Condensed Matter Physics</subject><subject>Covalence</subject><subject>Covalent bonds</subject><subject>Crystallography</subject><subject>Dielectric properties</subject><subject>Electric polarization</subject><subject>Ferrites</subject><subject>Ferroelectric materials</subject><subject>Ferroelectricity</subject><subject>Ferromagnetism</subject><subject>Functional groups</subject><subject>Heat treatment</subject><subject>Iron</subject><subject>Light emitting diodes</subject><subject>Machines</subject><subject>Magnetic saturation</subject><subject>Manufacturing</subject><subject>Materials science</subject><subject>Morphology</subject><subject>Muffle furnaces</subject><subject>Nanotechnology</subject><subject>Optical and Electronic Materials</subject><subject>Optical properties</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Powder metallurgy</subject><subject>Processes</subject><subject>Structural analysis</subject><subject>Surfaces and Interfaces</subject><subject>Thermal decomposition</subject><subject>Thin Films</subject><subject>Unit cell</subject><issn>0947-8396</issn><issn>1432-0630</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNp9kLFOHDEQhi0EEgfkBVJZogmFiT3ePa_LgLgQieiapLZsMw6Lbu3D9iLuCfLacXIgukzzS6Pvn5E-Qj4Kfik4V58L51JqxkEw3qklMH1AFqKTwPhS8kOy4LpTbJB6eUxOSnnkbTqABfm9SnmydUyRpkBjisxjrDmV3TRhzaOnPj3bTdtRl-J9ofcz0ppofUBaZlfqWOe3tk_ObmqLWBtf6Bjpd1Z3W6TO5nGe6AO-WBYw57FioVd2hZ8EsJeLtdBn5CjYTcEPr3lKfq5uflzfsrv112_XX-6YB8Urk0I6b7kOPQzKBucdggWnQIGznQiDhmCFRQsidDiA5ygaHbpeaq1lL0_J-f7uNqenGUs1j2nOsb000C_7QYBSslGwp3wzUTIGs83jZPPOCG7-Cjd74aYJN_-EG91Kcl8qDY6_ML-f_k_rD-t2hMk</recordid><startdate>20210901</startdate><enddate>20210901</enddate><creator>Sehar, Fatima</creator><creator>Anjum, Safia</creator><creator>Mansoor, Anam</creator><creator>Mustafa, Zeeshan</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20210901</creationdate><title>Formation of non-centrosymmetric covalent bonds due to the substitution of cobalt contents in M-type barium hexa-ferrites BaFe(12-x)O19</title><author>Sehar, Fatima ; Anjum, Safia ; Mansoor, Anam ; Mustafa, Zeeshan</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c270t-313bca09f5287afbcbe2a2b7272ba41f892fa1aea21f4e82c0e109ff453999353</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Applied physics</topic><topic>Barium</topic><topic>Characterization and Evaluation of Materials</topic><topic>Chemical bonds</topic><topic>Cobalt</topic><topic>Coercivity</topic><topic>Condensed Matter Physics</topic><topic>Covalence</topic><topic>Covalent bonds</topic><topic>Crystallography</topic><topic>Dielectric properties</topic><topic>Electric polarization</topic><topic>Ferrites</topic><topic>Ferroelectric materials</topic><topic>Ferroelectricity</topic><topic>Ferromagnetism</topic><topic>Functional groups</topic><topic>Heat treatment</topic><topic>Iron</topic><topic>Light emitting diodes</topic><topic>Machines</topic><topic>Magnetic saturation</topic><topic>Manufacturing</topic><topic>Materials science</topic><topic>Morphology</topic><topic>Muffle furnaces</topic><topic>Nanotechnology</topic><topic>Optical and Electronic Materials</topic><topic>Optical properties</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Powder metallurgy</topic><topic>Processes</topic><topic>Structural analysis</topic><topic>Surfaces and Interfaces</topic><topic>Thermal decomposition</topic><topic>Thin Films</topic><topic>Unit cell</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sehar, Fatima</creatorcontrib><creatorcontrib>Anjum, Safia</creatorcontrib><creatorcontrib>Mansoor, Anam</creatorcontrib><creatorcontrib>Mustafa, Zeeshan</creatorcontrib><collection>CrossRef</collection><jtitle>Applied physics. A, Materials science & processing</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sehar, Fatima</au><au>Anjum, Safia</au><au>Mansoor, Anam</au><au>Mustafa, Zeeshan</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Formation of non-centrosymmetric covalent bonds due to the substitution of cobalt contents in M-type barium hexa-ferrites BaFe(12-x)O19</atitle><jtitle>Applied physics. A, Materials science & processing</jtitle><stitle>Appl. Phys. A</stitle><date>2021-09-01</date><risdate>2021</risdate><volume>127</volume><issue>9</issue><artnum>718</artnum><issn>0947-8396</issn><eissn>1432-0630</eissn><abstract>The evolution of various properties of cobalt-doped M-type barium hexa-ferrites has been investigated in this project. A series of cobalt-doped M-type barium hexa-ferrites having general composition BaCo
x
Fe
(12-x)
O
19
with x = 0.2, 0.4, 0.6, 0.8, 1.0, and 1.2 was prepared using powder metallurgy route. For the thermal decomposition, prepared powders were heat-treated at 1373 K
o
for 2 h in a muffle furnace. The structural analysis, 3-D structural visualization, functional group analysis, surface morphology, elemental analysis, optical, dielectric, ferromagnetic, and ferroelectric properties of samples were characterized using different characterization techniques. X-ray diffractometer and Fourier transform infrared spectroscopy confirmed the formation of single-phase hexagonal structure of cobalt-doped M-type barium hexa-ferrite. The optical bandgap energy and saturation magnetization of the prepared samples increased with increasing cobalt concentration which made them suitable for light-emitting diodes and laser formation. Their dielectric properties show the insulting nature of the ferrites. Ferro-electric loop exhibits formation of non-centrosymmetric covalent bonds with an increase in the electric coercive field and remanent polarization. The electric polarization in the unit cell of barium hexa-ferrites is based on FeO6 octahedron. The oxygen O6 is located at three crystallographic sites (4f, 2a and 12 k). The iron ion is normally located at the center of the oxygen octahedron. The formation of non-centrosymmetric covalent bonds is due to the shifts off-center of iron ions under the application of external field. The ferroelectric loops are also not properly closed which indicates the magnetoelectric (ME) coupling and improves multiferroicity of the material.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1007/s00339-021-04762-9</doi></addata></record> |
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subjects | Applied physics Barium Characterization and Evaluation of Materials Chemical bonds Cobalt Coercivity Condensed Matter Physics Covalence Covalent bonds Crystallography Dielectric properties Electric polarization Ferrites Ferroelectric materials Ferroelectricity Ferromagnetism Functional groups Heat treatment Iron Light emitting diodes Machines Magnetic saturation Manufacturing Materials science Morphology Muffle furnaces Nanotechnology Optical and Electronic Materials Optical properties Physics Physics and Astronomy Powder metallurgy Processes Structural analysis Surfaces and Interfaces Thermal decomposition Thin Films Unit cell |
title | Formation of non-centrosymmetric covalent bonds due to the substitution of cobalt contents in M-type barium hexa-ferrites BaFe(12-x)O19 |
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