Effect of Ni doping on stabilization of Sm(Co1-xFex)5compound: thermodynamic calculation and experiment
The calculation of the heat of formation of Sm(Co1-x-yFexNiy)5compound using homemade software in the framework of Miedema's model was carried out. In addition we investigated the influence of the probability of occupation the transition metals sites by 3d-ions, in particular, equiprobable dist...
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creator | Gavrikov, I S Karpenkov, D Yu Zheleznyi, M V Kamynin, A V Khotulev, E S Bazlov, A I |
description | The calculation of the heat of formation of Sm(Co1-x-yFexNiy)5compound using homemade software in the framework of Miedema's model was carried out. In addition we investigated the influence of the probability of occupation the transition metals sites by 3d-ions, in particular, equiprobable distribution of 3d-ions among 2c and 3g sites and selective distribution Co/Ni-(2c), Fe-(3g). The maximal Fe and Ni doping ranges, where Sm(Co1-x-yFexNiy)5phase with the CaCu5-type crystal structure stable, were estimated for both types of distribution. The corresponding values of the number of 3d-electrons per atom were 7.23 (Fe/Co/Ni-(2c, 3g)) and 7.3 (Co/Ni-(2c), Fe-(3g)). Based on calculation the Sm(Co1-x-yFexNiy)5(x= 0.15, 0.3, 0.45;y= 0.05, 0.1, 0.15) melt-spun ribbons were synthesized. The maximal doping level ofx= 0.5 andy= 0.2 was experimentally determined for Fe and Ni atoms, respectively. These values are in good agreement with the theoretical prediction, assumed equiprobable distribution of 3d-ions among transition metal sites. The best among the series in terms of energy product Sm(Co0.6Fe0.3Ni0.1)5sample possesses a coercivity of 10.9 kOe and remanent magnetization of 51 emu g-1. |
doi_str_mv | 10.1088/1361-648X/aba0db |
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In addition we investigated the influence of the probability of occupation the transition metals sites by 3d-ions, in particular, equiprobable distribution of 3d-ions among 2c and 3g sites and selective distribution Co/Ni-(2c), Fe-(3g). The maximal Fe and Ni doping ranges, where Sm(Co1-x-yFexNiy)5phase with the CaCu5-type crystal structure stable, were estimated for both types of distribution. The corresponding values of the number of 3d-electrons per atom were 7.23 (Fe/Co/Ni-(2c, 3g)) and 7.3 (Co/Ni-(2c), Fe-(3g)). Based on calculation the Sm(Co1-x-yFexNiy)5(x= 0.15, 0.3, 0.45;y= 0.05, 0.1, 0.15) melt-spun ribbons were synthesized. The maximal doping level ofx= 0.5 andy= 0.2 was experimentally determined for Fe and Ni atoms, respectively. These values are in good agreement with the theoretical prediction, assumed equiprobable distribution of 3d-ions among transition metal sites. The best among the series in terms of energy product Sm(Co0.6Fe0.3Ni0.1)5sample possesses a coercivity of 10.9 kOe and remanent magnetization of 51 emu g-1.</description><identifier>EISSN: 1361-648X</identifier><identifier>DOI: 10.1088/1361-648X/aba0db</identifier><language>eng</language><ispartof>Journal of physics. 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In addition we investigated the influence of the probability of occupation the transition metals sites by 3d-ions, in particular, equiprobable distribution of 3d-ions among 2c and 3g sites and selective distribution Co/Ni-(2c), Fe-(3g). The maximal Fe and Ni doping ranges, where Sm(Co1-x-yFexNiy)5phase with the CaCu5-type crystal structure stable, were estimated for both types of distribution. The corresponding values of the number of 3d-electrons per atom were 7.23 (Fe/Co/Ni-(2c, 3g)) and 7.3 (Co/Ni-(2c), Fe-(3g)). Based on calculation the Sm(Co1-x-yFexNiy)5(x= 0.15, 0.3, 0.45;y= 0.05, 0.1, 0.15) melt-spun ribbons were synthesized. The maximal doping level ofx= 0.5 andy= 0.2 was experimentally determined for Fe and Ni atoms, respectively. These values are in good agreement with the theoretical prediction, assumed equiprobable distribution of 3d-ions among transition metal sites. The best among the series in terms of energy product Sm(Co0.6Fe0.3Ni0.1)5sample possesses a coercivity of 10.9 kOe and remanent magnetization of 51 emu g-1.</description><issn>1361-648X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNo9jMFLwzAYxYMgOKd3jznOQ13SNGnqTcamwtCDCt7G1-TLjLRJXVKY_vUOJp4e7_f4PUKuOLvhTOs5F4oXqtLvc2iB2faETP7RGTlP6ZMxVmlRTch26RyaTKOjT57aOPiwpTHQlKH1nf-B7A_tsL70s0XkxX6F-2tpYj_EMdhbmj9w10f7HaD3hhrozNgdHQiW4n7Ane8x5Aty6qBLePmXU_K2Wr4uHor18_3j4m5dDJyJXGhpbMvKugR0rJKoGlk3qJUUDVetFlagNKJ2ldYooFVaugZ0KZgyCNY4MSWz4--wi18jprzpfTLYdRAwjmlTVrxhWtVMiF-0UFqV</recordid><startdate>20201007</startdate><enddate>20201007</enddate><creator>Gavrikov, I S</creator><creator>Karpenkov, D Yu</creator><creator>Zheleznyi, M V</creator><creator>Kamynin, A V</creator><creator>Khotulev, E S</creator><creator>Bazlov, A I</creator><scope>7X8</scope></search><sort><creationdate>20201007</creationdate><title>Effect of Ni doping on stabilization of Sm(Co1-xFex)5compound: thermodynamic calculation and experiment</title><author>Gavrikov, I S ; Karpenkov, D Yu ; Zheleznyi, M V ; Kamynin, A V ; Khotulev, E S ; Bazlov, A I</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p103t-85cdb0272aef045e69579e8653916b83d3e5c37f488e3ab685f9a82306ceadcf3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Gavrikov, I S</creatorcontrib><creatorcontrib>Karpenkov, D Yu</creatorcontrib><creatorcontrib>Zheleznyi, M V</creatorcontrib><creatorcontrib>Kamynin, A V</creatorcontrib><creatorcontrib>Khotulev, E S</creatorcontrib><creatorcontrib>Bazlov, A I</creatorcontrib><collection>MEDLINE - Academic</collection><jtitle>Journal of physics. Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gavrikov, I S</au><au>Karpenkov, D Yu</au><au>Zheleznyi, M V</au><au>Kamynin, A V</au><au>Khotulev, E S</au><au>Bazlov, A I</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of Ni doping on stabilization of Sm(Co1-xFex)5compound: thermodynamic calculation and experiment</atitle><jtitle>Journal of physics. Condensed matter</jtitle><date>2020-10-07</date><risdate>2020</risdate><volume>32</volume><issue>42</issue><eissn>1361-648X</eissn><abstract>The calculation of the heat of formation of Sm(Co1-x-yFexNiy)5compound using homemade software in the framework of Miedema's model was carried out. In addition we investigated the influence of the probability of occupation the transition metals sites by 3d-ions, in particular, equiprobable distribution of 3d-ions among 2c and 3g sites and selective distribution Co/Ni-(2c), Fe-(3g). The maximal Fe and Ni doping ranges, where Sm(Co1-x-yFexNiy)5phase with the CaCu5-type crystal structure stable, were estimated for both types of distribution. The corresponding values of the number of 3d-electrons per atom were 7.23 (Fe/Co/Ni-(2c, 3g)) and 7.3 (Co/Ni-(2c), Fe-(3g)). Based on calculation the Sm(Co1-x-yFexNiy)5(x= 0.15, 0.3, 0.45;y= 0.05, 0.1, 0.15) melt-spun ribbons were synthesized. The maximal doping level ofx= 0.5 andy= 0.2 was experimentally determined for Fe and Ni atoms, respectively. These values are in good agreement with the theoretical prediction, assumed equiprobable distribution of 3d-ions among transition metal sites. The best among the series in terms of energy product Sm(Co0.6Fe0.3Ni0.1)5sample possesses a coercivity of 10.9 kOe and remanent magnetization of 51 emu g-1.</abstract><doi>10.1088/1361-648X/aba0db</doi></addata></record> |
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title | Effect of Ni doping on stabilization of Sm(Co1-xFex)5compound: thermodynamic calculation and experiment |
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