Structural and Magnetic Behavior of BaAl{sub x}Cr{sub y}Fe{sub 11}O{sub 19} (x + y = 1) Hexagonal Ferrites
The present study aims to analyze barium hexagonal ferrite and its derivation behavior using sol-gel auto-combustion co-doped with Al{sup 3+}/Cr{sup 3+}ions. Also, the effects of dopants on structural and magnetic properties of prepared samples were investigated. To this purpose, the finest powders...
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Veröffentlicht in: | Journal of superconductivity and novel magnetism 2019-08, Vol.32 (8) |
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creator | Alimoradi, M. Yousefi, M. Sadeghi, B. Amini, M. M. Abbasi, A. |
description | The present study aims to analyze barium hexagonal ferrite and its derivation behavior using sol-gel auto-combustion co-doped with Al{sup 3+}/Cr{sup 3+}ions. Also, the effects of dopants on structural and magnetic properties of prepared samples were investigated. To this purpose, the finest powders were preheated at 500 °C for 1 h and calcinated at 900 °C about 2 h. Then, the magnetic powders were characterized by Fourier transform infrared spectroscopy (FTIR), X-ray diffraction (XRD), field emission scanning electron microscope (FESEM), and vibrating sample magnetometer (VSM). The XRD patterns show the magnetoplumbite phase. According to the Scherrer equation applied, inserting ions led to a decrease in lattice parameters (a and c) and crystallite size. The morphology of synthesized samples was observed by FESEM and proved the hexagonal shapes of the prepared samples. The nanoparticles sizes were recorded between 59 and 79 nm. Moreover, the magnetic properties of prepared samples were specified by VSM. The saturation magnetization (M{sub s}) and remnant magnetization (M{sub r}) of the synthesized magnetic powders were decreased by inserting Al{sup 3+}/Cr{sup 3+} ions, while coercivity (H{sub c}) increased from 5215 to 7178 Oe. . |
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M. ; Abbasi, A.</creator><creatorcontrib>Alimoradi, M. ; Yousefi, M. ; Sadeghi, B. ; Amini, M. M. ; Abbasi, A.</creatorcontrib><description>The present study aims to analyze barium hexagonal ferrite and its derivation behavior using sol-gel auto-combustion co-doped with Al{sup 3+}/Cr{sup 3+}ions. Also, the effects of dopants on structural and magnetic properties of prepared samples were investigated. To this purpose, the finest powders were preheated at 500 °C for 1 h and calcinated at 900 °C about 2 h. Then, the magnetic powders were characterized by Fourier transform infrared spectroscopy (FTIR), X-ray diffraction (XRD), field emission scanning electron microscope (FESEM), and vibrating sample magnetometer (VSM). The XRD patterns show the magnetoplumbite phase. According to the Scherrer equation applied, inserting ions led to a decrease in lattice parameters (a and c) and crystallite size. The morphology of synthesized samples was observed by FESEM and proved the hexagonal shapes of the prepared samples. The nanoparticles sizes were recorded between 59 and 79 nm. Moreover, the magnetic properties of prepared samples were specified by VSM. The saturation magnetization (M{sub s}) and remnant magnetization (M{sub r}) of the synthesized magnetic powders were decreased by inserting Al{sup 3+}/Cr{sup 3+} ions, while coercivity (H{sub c}) increased from 5215 to 7178 Oe. .</description><identifier>ISSN: 1557-1939</identifier><identifier>EISSN: 1557-1947</identifier><language>eng</language><publisher>United States</publisher><subject>ALUMINIUM ADDITIONS ; BARIUM COMPOUNDS ; CHROMIUM ADDITIONS ; COERCIVE FORCE ; DOPED MATERIALS ; FERRITES ; FIELD EMISSION ; FOURIER TRANSFORM SPECTROMETERS ; FOURIER TRANSFORMATION ; INFRARED SPECTRA ; LATTICE PARAMETERS ; MAGNETIC PROPERTIES ; MAGNETIZATION ; NANOCOMPOSITES ; NANOPARTICLES ; NANOSCIENCE AND NANOTECHNOLOGY ; SCANNING ELECTRON MICROSCOPY ; SOL-GEL PROCESS ; VIBRATING SAMPLE MAGNETOMETERS ; X-RAY DIFFRACTION</subject><ispartof>Journal of superconductivity and novel magnetism, 2019-08, Vol.32 (8)</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22922952$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Alimoradi, M.</creatorcontrib><creatorcontrib>Yousefi, M.</creatorcontrib><creatorcontrib>Sadeghi, B.</creatorcontrib><creatorcontrib>Amini, M. M.</creatorcontrib><creatorcontrib>Abbasi, A.</creatorcontrib><title>Structural and Magnetic Behavior of BaAl{sub x}Cr{sub y}Fe{sub 11}O{sub 19} (x + y = 1) Hexagonal Ferrites</title><title>Journal of superconductivity and novel magnetism</title><description>The present study aims to analyze barium hexagonal ferrite and its derivation behavior using sol-gel auto-combustion co-doped with Al{sup 3+}/Cr{sup 3+}ions. Also, the effects of dopants on structural and magnetic properties of prepared samples were investigated. To this purpose, the finest powders were preheated at 500 °C for 1 h and calcinated at 900 °C about 2 h. Then, the magnetic powders were characterized by Fourier transform infrared spectroscopy (FTIR), X-ray diffraction (XRD), field emission scanning electron microscope (FESEM), and vibrating sample magnetometer (VSM). The XRD patterns show the magnetoplumbite phase. According to the Scherrer equation applied, inserting ions led to a decrease in lattice parameters (a and c) and crystallite size. The morphology of synthesized samples was observed by FESEM and proved the hexagonal shapes of the prepared samples. The nanoparticles sizes were recorded between 59 and 79 nm. Moreover, the magnetic properties of prepared samples were specified by VSM. The saturation magnetization (M{sub s}) and remnant magnetization (M{sub r}) of the synthesized magnetic powders were decreased by inserting Al{sup 3+}/Cr{sup 3+} ions, while coercivity (H{sub c}) increased from 5215 to 7178 Oe. .</description><subject>ALUMINIUM ADDITIONS</subject><subject>BARIUM COMPOUNDS</subject><subject>CHROMIUM ADDITIONS</subject><subject>COERCIVE FORCE</subject><subject>DOPED MATERIALS</subject><subject>FERRITES</subject><subject>FIELD EMISSION</subject><subject>FOURIER TRANSFORM SPECTROMETERS</subject><subject>FOURIER TRANSFORMATION</subject><subject>INFRARED SPECTRA</subject><subject>LATTICE PARAMETERS</subject><subject>MAGNETIC PROPERTIES</subject><subject>MAGNETIZATION</subject><subject>NANOCOMPOSITES</subject><subject>NANOPARTICLES</subject><subject>NANOSCIENCE AND NANOTECHNOLOGY</subject><subject>SCANNING ELECTRON MICROSCOPY</subject><subject>SOL-GEL PROCESS</subject><subject>VIBRATING SAMPLE MAGNETOMETERS</subject><subject>X-RAY DIFFRACTION</subject><issn>1557-1939</issn><issn>1557-1947</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNpjYuA0NDU11zW0NDFngbONLTkYuIqLswwMTEyNDcw4GYqCS4pKk0tKixJzFBLzUhR8E9PzUksykxWcUjMSyzLzixTy0xScEh1zqotLkxQqap2LwIzKWrdUMMPQsNYfwrCsVdCoeNTQqQ3ElUBsC8SGmgoeqRWJ6fl5QOPdUouKMktSi3kYWNMSc4pTeaE0N4Oym2uIs4dufnFJZnxxMlBNckZyfl5eanJJvJGRJRCZGhkTpwoAsNZPPw</recordid><startdate>20190815</startdate><enddate>20190815</enddate><creator>Alimoradi, M.</creator><creator>Yousefi, M.</creator><creator>Sadeghi, B.</creator><creator>Amini, M. M.</creator><creator>Abbasi, A.</creator><scope>OTOTI</scope></search><sort><creationdate>20190815</creationdate><title>Structural and Magnetic Behavior of BaAl{sub x}Cr{sub y}Fe{sub 11}O{sub 19} (x + y = 1) Hexagonal Ferrites</title><author>Alimoradi, M. ; Yousefi, M. ; Sadeghi, B. ; Amini, M. 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M.</creatorcontrib><creatorcontrib>Abbasi, A.</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Journal of superconductivity and novel magnetism</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Alimoradi, M.</au><au>Yousefi, M.</au><au>Sadeghi, B.</au><au>Amini, M. M.</au><au>Abbasi, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structural and Magnetic Behavior of BaAl{sub x}Cr{sub y}Fe{sub 11}O{sub 19} (x + y = 1) Hexagonal Ferrites</atitle><jtitle>Journal of superconductivity and novel magnetism</jtitle><date>2019-08-15</date><risdate>2019</risdate><volume>32</volume><issue>8</issue><issn>1557-1939</issn><eissn>1557-1947</eissn><abstract>The present study aims to analyze barium hexagonal ferrite and its derivation behavior using sol-gel auto-combustion co-doped with Al{sup 3+}/Cr{sup 3+}ions. Also, the effects of dopants on structural and magnetic properties of prepared samples were investigated. To this purpose, the finest powders were preheated at 500 °C for 1 h and calcinated at 900 °C about 2 h. Then, the magnetic powders were characterized by Fourier transform infrared spectroscopy (FTIR), X-ray diffraction (XRD), field emission scanning electron microscope (FESEM), and vibrating sample magnetometer (VSM). The XRD patterns show the magnetoplumbite phase. According to the Scherrer equation applied, inserting ions led to a decrease in lattice parameters (a and c) and crystallite size. The morphology of synthesized samples was observed by FESEM and proved the hexagonal shapes of the prepared samples. The nanoparticles sizes were recorded between 59 and 79 nm. Moreover, the magnetic properties of prepared samples were specified by VSM. The saturation magnetization (M{sub s}) and remnant magnetization (M{sub r}) of the synthesized magnetic powders were decreased by inserting Al{sup 3+}/Cr{sup 3+} ions, while coercivity (H{sub c}) increased from 5215 to 7178 Oe. .</abstract><cop>United States</cop></addata></record> |
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subjects | ALUMINIUM ADDITIONS BARIUM COMPOUNDS CHROMIUM ADDITIONS COERCIVE FORCE DOPED MATERIALS FERRITES FIELD EMISSION FOURIER TRANSFORM SPECTROMETERS FOURIER TRANSFORMATION INFRARED SPECTRA LATTICE PARAMETERS MAGNETIC PROPERTIES MAGNETIZATION NANOCOMPOSITES NANOPARTICLES NANOSCIENCE AND NANOTECHNOLOGY SCANNING ELECTRON MICROSCOPY SOL-GEL PROCESS VIBRATING SAMPLE MAGNETOMETERS X-RAY DIFFRACTION |
title | Structural and Magnetic Behavior of BaAl{sub x}Cr{sub y}Fe{sub 11}O{sub 19} (x + y = 1) Hexagonal Ferrites |
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