Effect of Valence Floating on the Magnetic Properties of Ca-Sn Co-Doping Y3−xCaxFe5−xSnxO12(x = 0-0.25)
First-principle calculations were used to simulate the changes in magnetic parameters and interatomic charge density in the crystal structure of yttrium iron garnet (YIG) caused by Ca-Sn co-doping. The simulation results illustrate that Ca and Sn have no spin polarization in the crystal, and the cha...
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description | First-principle calculations were used to simulate the changes in magnetic parameters and interatomic charge density in the crystal structure of yttrium iron garnet (YIG) caused by Ca-Sn co-doping. The simulation results illustrate that Ca and Sn have no spin polarization in the crystal, and the charge density among ions tends to increase with doping concentration. A solid-state reaction method was employed to prepare YIG with varying concentrations of Ca-Sn co-doping. The saturation magnetization ( 4\pi M_{s} ) of the material shows an initial increase and then decrease as the number of doping increases. This phenomenon of increment in 4\pi M_{s} at first could be accounted for the increase of the net magnetic moment of material. The reduction in 4\pi M_{s} could be interpreted as the content of Fe 3+ ( 5~\mu \text{B} ) decreases, while the Fe 2+ ( 4~\mu \text{B} ) in the material becomes the primary portion when the concentration of doping exceeds 0.10. |
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The simulation results illustrate that Ca and Sn have no spin polarization in the crystal, and the charge density among ions tends to increase with doping concentration. A solid-state reaction method was employed to prepare YIG with varying concentrations of Ca-Sn co-doping. The saturation magnetization (<inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula>) of the material shows an initial increase and then decrease as the number of doping increases. This phenomenon of increment in <inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula> at first could be accounted for the increase of the net magnetic moment of material. The reduction in <inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula> could be interpreted as the content of Fe 3+ (<inline-formula> <tex-math notation="LaTeX">5~\mu \text{B} </tex-math></inline-formula>) decreases, while the Fe 2+ (<inline-formula> <tex-math notation="LaTeX">4~\mu \text{B} </tex-math></inline-formula>) in the material becomes the primary portion when the concentration of doping exceeds 0.10.]]></description><identifier>ISSN: 0018-9464</identifier><identifier>EISSN: 1941-0069</identifier><identifier>DOI: 10.1109/TMAG.2022.3179106</identifier><identifier>CODEN: IEMGAQ</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Ca–Sn co-doping ; Ceramics ; Charge density ; Crystal structure ; Crystals ; density functional theory (DFT) ; Doping ; Ferrites ; First principles ; garnet-type ferrites ; Ions ; Iron ; Magnetic moments ; Magnetic properties ; Magnetic saturation ; Magnetism ; perovskite ; Polarization (spin alignment) ; Saturation magnetization ; yttrium iron garnet (YIG) ceramics ; Yttrium-iron garnet</subject><ispartof>IEEE transactions on magnetics, 2022-08, Vol.58 (8), p.1-5</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2022</rights><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c251t-f062086af7b32bd680319ddb010cfe9e391246fd47ec832da2429549c45d955c3</citedby><orcidid>0000-0001-5081-7893 ; 0000-0002-1019-1168 ; 0000-0003-2866-5234</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/9785628$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27923,27924,54757</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/9785628$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Yin, Qisheng</creatorcontrib><creatorcontrib>Liu, Yingli</creatorcontrib><creatorcontrib>Chen, Jianfeng</creatorcontrib><creatorcontrib>Lu, Shifan</creatorcontrib><title>Effect of Valence Floating on the Magnetic Properties of Ca-Sn Co-Doping Y3−xCaxFe5−xSnxO12(x = 0-0.25)</title><title>IEEE transactions on magnetics</title><addtitle>TMAG</addtitle><description><![CDATA[First-principle calculations were used to simulate the changes in magnetic parameters and interatomic charge density in the crystal structure of yttrium iron garnet (YIG) caused by Ca-Sn co-doping. The simulation results illustrate that Ca and Sn have no spin polarization in the crystal, and the charge density among ions tends to increase with doping concentration. A solid-state reaction method was employed to prepare YIG with varying concentrations of Ca-Sn co-doping. The saturation magnetization (<inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula>) of the material shows an initial increase and then decrease as the number of doping increases. This phenomenon of increment in <inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula> at first could be accounted for the increase of the net magnetic moment of material. The reduction in <inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula> could be interpreted as the content of Fe 3+ (<inline-formula> <tex-math notation="LaTeX">5~\mu \text{B} </tex-math></inline-formula>) decreases, while the Fe 2+ (<inline-formula> <tex-math notation="LaTeX">4~\mu \text{B} </tex-math></inline-formula>) in the material becomes the primary portion when the concentration of doping exceeds 0.10.]]></description><subject>Ca–Sn co-doping</subject><subject>Ceramics</subject><subject>Charge density</subject><subject>Crystal structure</subject><subject>Crystals</subject><subject>density functional theory (DFT)</subject><subject>Doping</subject><subject>Ferrites</subject><subject>First principles</subject><subject>garnet-type ferrites</subject><subject>Ions</subject><subject>Iron</subject><subject>Magnetic moments</subject><subject>Magnetic properties</subject><subject>Magnetic saturation</subject><subject>Magnetism</subject><subject>perovskite</subject><subject>Polarization (spin alignment)</subject><subject>Saturation magnetization</subject><subject>yttrium iron garnet (YIG) ceramics</subject><subject>Yttrium-iron garnet</subject><issn>0018-9464</issn><issn>1941-0069</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNotzc1Kw0AUBeBBFKzVBxA3A250MfHObzILFxLbKrRUaBVchelkpqbWTExSiG_g2kf0SWypq3sOfJyL0DmFiFLQN_PJ3ShiwFjEaawpqAPUo1pQAqD0IeoB0IRoocQxOmma1bYKSaGH3gfeO9vi4PGLWbvSOjxcB9MW5RKHErdvDk_MsnRtYfFTHSpXt4Vrdjw1ZFbiNJD7UO30K__9_ulS0w2d3KVZ2U0pu-rwLQYCEZPXp-jIm3Xjzv5vHz0PB_P0gYyno8f0bkwsk7QlHhSDRBkfLzhb5CoBTnWeL4CC9U47rikTyucidjbhLDdMMC2FtkLmWkrL--hyv1vV4XPjmjZbhU1dbl9mTGlJJVMy2aqLvSqcc1lVFx-m_sp0nEjFEv4HsBhhWw</recordid><startdate>20220801</startdate><enddate>20220801</enddate><creator>Yin, Qisheng</creator><creator>Liu, Yingli</creator><creator>Chen, Jianfeng</creator><creator>Lu, Shifan</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>7SP</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-5081-7893</orcidid><orcidid>https://orcid.org/0000-0002-1019-1168</orcidid><orcidid>https://orcid.org/0000-0003-2866-5234</orcidid></search><sort><creationdate>20220801</creationdate><title>Effect of Valence Floating on the Magnetic Properties of Ca-Sn Co-Doping Y3−xCaxFe5−xSnxO12(x = 0-0.25)</title><author>Yin, Qisheng ; Liu, Yingli ; Chen, Jianfeng ; Lu, Shifan</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c251t-f062086af7b32bd680319ddb010cfe9e391246fd47ec832da2429549c45d955c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Ca–Sn co-doping</topic><topic>Ceramics</topic><topic>Charge density</topic><topic>Crystal structure</topic><topic>Crystals</topic><topic>density functional theory (DFT)</topic><topic>Doping</topic><topic>Ferrites</topic><topic>First principles</topic><topic>garnet-type ferrites</topic><topic>Ions</topic><topic>Iron</topic><topic>Magnetic moments</topic><topic>Magnetic properties</topic><topic>Magnetic saturation</topic><topic>Magnetism</topic><topic>perovskite</topic><topic>Polarization (spin alignment)</topic><topic>Saturation magnetization</topic><topic>yttrium iron garnet (YIG) ceramics</topic><topic>Yttrium-iron garnet</topic><toplevel>online_resources</toplevel><creatorcontrib>Yin, Qisheng</creatorcontrib><creatorcontrib>Liu, Yingli</creatorcontrib><creatorcontrib>Chen, Jianfeng</creatorcontrib><creatorcontrib>Lu, Shifan</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>Electronics & Communications 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>IEEE transactions on magnetics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Yin, Qisheng</au><au>Liu, Yingli</au><au>Chen, Jianfeng</au><au>Lu, Shifan</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of Valence Floating on the Magnetic Properties of Ca-Sn Co-Doping Y3−xCaxFe5−xSnxO12(x = 0-0.25)</atitle><jtitle>IEEE transactions on magnetics</jtitle><stitle>TMAG</stitle><date>2022-08-01</date><risdate>2022</risdate><volume>58</volume><issue>8</issue><spage>1</spage><epage>5</epage><pages>1-5</pages><issn>0018-9464</issn><eissn>1941-0069</eissn><coden>IEMGAQ</coden><abstract><![CDATA[First-principle calculations were used to simulate the changes in magnetic parameters and interatomic charge density in the crystal structure of yttrium iron garnet (YIG) caused by Ca-Sn co-doping. The simulation results illustrate that Ca and Sn have no spin polarization in the crystal, and the charge density among ions tends to increase with doping concentration. A solid-state reaction method was employed to prepare YIG with varying concentrations of Ca-Sn co-doping. The saturation magnetization (<inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula>) of the material shows an initial increase and then decrease as the number of doping increases. This phenomenon of increment in <inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula> at first could be accounted for the increase of the net magnetic moment of material. The reduction in <inline-formula> <tex-math notation="LaTeX">4\pi M_{s} </tex-math></inline-formula> could be interpreted as the content of Fe 3+ (<inline-formula> <tex-math notation="LaTeX">5~\mu \text{B} </tex-math></inline-formula>) decreases, while the Fe 2+ (<inline-formula> <tex-math notation="LaTeX">4~\mu \text{B} </tex-math></inline-formula>) in the material becomes the primary portion when the concentration of doping exceeds 0.10.]]></abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TMAG.2022.3179106</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0001-5081-7893</orcidid><orcidid>https://orcid.org/0000-0002-1019-1168</orcidid><orcidid>https://orcid.org/0000-0003-2866-5234</orcidid></addata></record> |
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subjects | Ca–Sn co-doping Ceramics Charge density Crystal structure Crystals density functional theory (DFT) Doping Ferrites First principles garnet-type ferrites Ions Iron Magnetic moments Magnetic properties Magnetic saturation Magnetism perovskite Polarization (spin alignment) Saturation magnetization yttrium iron garnet (YIG) ceramics Yttrium-iron garnet |
title | Effect of Valence Floating on the Magnetic Properties of Ca-Sn Co-Doping Y3−xCaxFe5−xSnxO12(x = 0-0.25) |
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