Structural and Magnetic Properties of (Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 Spinel Solid Solution Obtained by Molten Salt Synthesis

(Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 (x = 0.0, 0.4, 0.8, 1.2, and 1.6) spinel particles are prepared by molten salt method at 1050 °C for 5 h. The solid solution structure is determined by X‐ray diffraction (XRD) as cubic spinel with Fd‐3m space group. The lattice parameter and crystalline size decre...

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Veröffentlicht in:Physica status solidi. A, Applications and materials science Applications and materials science, 2021-04, Vol.218 (7), p.n/a
Hauptverfasser: Wu, Xingrong, Pan, Tiantian, Shen, Xingmei, Cao, Fabin, Wu, Zhaojin
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Pan, Tiantian
Shen, Xingmei
Cao, Fabin
Wu, Zhaojin
description (Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 (x = 0.0, 0.4, 0.8, 1.2, and 1.6) spinel particles are prepared by molten salt method at 1050 °C for 5 h. The solid solution structure is determined by X‐ray diffraction (XRD) as cubic spinel with Fd‐3m space group. The lattice parameter and crystalline size decrease with increasing Cr content. Cr3+ ions occupy the octahedral sites, as shown by combined Fourier transform infrared spectroscopy (FTIR) and XRD analysis. The magnetization as a function of field (±4.52 T) and field‐cooled (FC) and zero‐field‐cooled (ZFC) magnetization measurements under a field of 100 Oe is measured for temperatures ranging from 1.5 to 300 K. It is found from M(T) curves that the interparticle interactions are suppressed below 28.1–40.8 K, and the curves also shows the ferromagnetic from M(H) hysteresis for the samples with x = 0.0, 0.4, and 0.8. However, for x = 1.2 and 1.6, the samples show superparamagnetic, as also supported by the obtained electron paramagnetic resonance (EPR) and Mössbauer spectra. (Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 particles are prepared by molten salt method. A single‐phase spinel solid solution is formed for x = 0.0–1.2. The lattice constant and particle size decrease with increasing chromium content. Interparticle interactions are suppressed below 28.1–40.8 K, and the samples show ferromagnetic behavior for x = 0.0, 0.4, 0.8, while superparamagnetic for x = 1.2, 1.6.
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The solid solution structure is determined by X‐ray diffraction (XRD) as cubic spinel with Fd‐3m space group. The lattice parameter and crystalline size decrease with increasing Cr content. Cr3+ ions occupy the octahedral sites, as shown by combined Fourier transform infrared spectroscopy (FTIR) and XRD analysis. The magnetization as a function of field (±4.52 T) and field‐cooled (FC) and zero‐field‐cooled (ZFC) magnetization measurements under a field of 100 Oe is measured for temperatures ranging from 1.5 to 300 K. It is found from M(T) curves that the interparticle interactions are suppressed below 28.1–40.8 K, and the curves also shows the ferromagnetic from M(H) hysteresis for the samples with x = 0.0, 0.4, and 0.8. However, for x = 1.2 and 1.6, the samples show superparamagnetic, as also supported by the obtained electron paramagnetic resonance (EPR) and Mössbauer spectra. (Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 particles are prepared by molten salt method. A single‐phase spinel solid solution is formed for x = 0.0–1.2. The lattice constant and particle size decrease with increasing chromium content. Interparticle interactions are suppressed below 28.1–40.8 K, and the samples show ferromagnetic behavior for x = 0.0, 0.4, 0.8, while superparamagnetic for x = 1.2, 1.6.</description><identifier>ISSN: 1862-6300</identifier><identifier>EISSN: 1862-6319</identifier><identifier>DOI: 10.1002/pssa.202000518</identifier><language>eng</language><publisher>Weinheim: Wiley Subscription Services, Inc</publisher><subject>Chromium ; Crystals ; Cubic lattice ; Electron paramagnetic resonance ; Ferromagnetism ; Fourier transforms ; Infrared analysis ; Magnetic properties ; Magnetization ; molten salt synthesis ; Molten salts ; Solid solutions ; Spectrum analysis ; Spinel ; spinels ; superparamagnetic ; X-ray diffraction</subject><ispartof>Physica status solidi. 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A, Applications and materials science</title><description>(Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 (x = 0.0, 0.4, 0.8, 1.2, and 1.6) spinel particles are prepared by molten salt method at 1050 °C for 5 h. The solid solution structure is determined by X‐ray diffraction (XRD) as cubic spinel with Fd‐3m space group. The lattice parameter and crystalline size decrease with increasing Cr content. Cr3+ ions occupy the octahedral sites, as shown by combined Fourier transform infrared spectroscopy (FTIR) and XRD analysis. The magnetization as a function of field (±4.52 T) and field‐cooled (FC) and zero‐field‐cooled (ZFC) magnetization measurements under a field of 100 Oe is measured for temperatures ranging from 1.5 to 300 K. It is found from M(T) curves that the interparticle interactions are suppressed below 28.1–40.8 K, and the curves also shows the ferromagnetic from M(H) hysteresis for the samples with x = 0.0, 0.4, and 0.8. 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Interparticle interactions are suppressed below 28.1–40.8 K, and the samples show ferromagnetic behavior for x = 0.0, 0.4, 0.8, while superparamagnetic for x = 1.2, 1.6.</description><subject>Chromium</subject><subject>Crystals</subject><subject>Cubic lattice</subject><subject>Electron paramagnetic resonance</subject><subject>Ferromagnetism</subject><subject>Fourier transforms</subject><subject>Infrared analysis</subject><subject>Magnetic properties</subject><subject>Magnetization</subject><subject>molten salt synthesis</subject><subject>Molten salts</subject><subject>Solid solutions</subject><subject>Spectrum analysis</subject><subject>Spinel</subject><subject>spinels</subject><subject>superparamagnetic</subject><subject>X-ray diffraction</subject><issn>1862-6300</issn><issn>1862-6319</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNo9kEFLw0AQhYMoWKtXzwteWkri7GaTTY6lWBVaWoiew6aZ1JQ1ibsbbM5ePPsT_SWmVHqZN294vIHPcW4peBSA3TfGSI8BA4CARmfOgEYhc0OfxuenHeDSuTJmB8ADLujA-Uqsbje21VIRWeVkKbcV2nJD1rpuUNsSDakLMlpuwYvmyCbgsfFoqsDjM72foz-hXvj7_bMfrzhJmrJCRZJalflhtrasK7LKrOzvOck6sqyVxYokUlmSdJV9Q1Oaa-eikMrgzb8Ondf5w8vsyV2sHp9n04XbUB5FbsTDMEcBEfeBYyFEEFHAOMNMZFRkGItMhBxDziEo_LC3yAFi5LGMKRS5P3Tujr2Nrj9aNDbd1a2u-pcpCyBmlAka9Kn4mPosFXZpo8t3qbuUQnqgnB4opyfK6TpJpifn_wFJwXEm</recordid><startdate>202104</startdate><enddate>202104</enddate><creator>Wu, Xingrong</creator><creator>Pan, Tiantian</creator><creator>Shen, Xingmei</creator><creator>Cao, Fabin</creator><creator>Wu, Zhaojin</creator><general>Wiley Subscription Services, Inc</general><scope>7SP</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-3676-549X</orcidid></search><sort><creationdate>202104</creationdate><title>Structural and Magnetic Properties of (Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 Spinel Solid Solution Obtained by Molten Salt Synthesis</title><author>Wu, Xingrong ; Pan, Tiantian ; Shen, Xingmei ; Cao, Fabin ; Wu, Zhaojin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p1488-8466de7084304ef775810e9beb7b17be97b764e64405f3697be4009e49a910fd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Chromium</topic><topic>Crystals</topic><topic>Cubic lattice</topic><topic>Electron paramagnetic resonance</topic><topic>Ferromagnetism</topic><topic>Fourier transforms</topic><topic>Infrared analysis</topic><topic>Magnetic properties</topic><topic>Magnetization</topic><topic>molten salt synthesis</topic><topic>Molten salts</topic><topic>Solid solutions</topic><topic>Spectrum analysis</topic><topic>Spinel</topic><topic>spinels</topic><topic>superparamagnetic</topic><topic>X-ray diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wu, Xingrong</creatorcontrib><creatorcontrib>Pan, Tiantian</creatorcontrib><creatorcontrib>Shen, Xingmei</creatorcontrib><creatorcontrib>Cao, Fabin</creatorcontrib><creatorcontrib>Wu, Zhaojin</creatorcontrib><collection>Electronics &amp; Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physica status solidi. A, Applications and materials science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wu, Xingrong</au><au>Pan, Tiantian</au><au>Shen, Xingmei</au><au>Cao, Fabin</au><au>Wu, Zhaojin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structural and Magnetic Properties of (Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 Spinel Solid Solution Obtained by Molten Salt Synthesis</atitle><jtitle>Physica status solidi. A, Applications and materials science</jtitle><date>2021-04</date><risdate>2021</risdate><volume>218</volume><issue>7</issue><epage>n/a</epage><issn>1862-6300</issn><eissn>1862-6319</eissn><abstract>(Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 (x = 0.0, 0.4, 0.8, 1.2, and 1.6) spinel particles are prepared by molten salt method at 1050 °C for 5 h. The solid solution structure is determined by X‐ray diffraction (XRD) as cubic spinel with Fd‐3m space group. The lattice parameter and crystalline size decrease with increasing Cr content. Cr3+ ions occupy the octahedral sites, as shown by combined Fourier transform infrared spectroscopy (FTIR) and XRD analysis. The magnetization as a function of field (±4.52 T) and field‐cooled (FC) and zero‐field‐cooled (ZFC) magnetization measurements under a field of 100 Oe is measured for temperatures ranging from 1.5 to 300 K. It is found from M(T) curves that the interparticle interactions are suppressed below 28.1–40.8 K, and the curves also shows the ferromagnetic from M(H) hysteresis for the samples with x = 0.0, 0.4, and 0.8. However, for x = 1.2 and 1.6, the samples show superparamagnetic, as also supported by the obtained electron paramagnetic resonance (EPR) and Mössbauer spectra. (Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 particles are prepared by molten salt method. A single‐phase spinel solid solution is formed for x = 0.0–1.2. The lattice constant and particle size decrease with increasing chromium content. Interparticle interactions are suppressed below 28.1–40.8 K, and the samples show ferromagnetic behavior for x = 0.0, 0.4, 0.8, while superparamagnetic for x = 1.2, 1.6.</abstract><cop>Weinheim</cop><pub>Wiley Subscription Services, Inc</pub><doi>10.1002/pssa.202000518</doi><tpages>9</tpages><orcidid>https://orcid.org/0000-0002-3676-549X</orcidid></addata></record>
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subjects Chromium
Crystals
Cubic lattice
Electron paramagnetic resonance
Ferromagnetism
Fourier transforms
Infrared analysis
Magnetic properties
Magnetization
molten salt synthesis
Molten salts
Solid solutions
Spectrum analysis
Spinel
spinels
superparamagnetic
X-ray diffraction
title Structural and Magnetic Properties of (Mg0.8Fe2+0.2)(Al0.4CrxFe3+1.6−x)O4 Spinel Solid Solution Obtained by Molten Salt Synthesis
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