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Anisotropic Nd-Fe-M-B flakes by single-roller melt spinning
Anisotropic Nd13Fe81−xMxB6 flakes (M=0.5–3 at. % one of Ti/Zr/V/Ta/Mo/Zn) are reproducibly obtainable using single-roller melt spinning at lower substrate velocities (Vs, 8–15 m/s). The degree of preferred orientation (DPO) of spun flakes calculated from x-ray diffraction patterns is 70%–97% on the...
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Published in: | Applied physics letters 1991-10, Vol.59 (16), p.2046-2048 |
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container_title | Applied physics letters |
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creator | TSUNG-SHUNE CHIN HUANG, S. H YAU, J. M |
description | Anisotropic Nd13Fe81−xMxB6 flakes (M=0.5–3 at. % one of Ti/Zr/V/Ta/Mo/Zn) are reproducibly obtainable using single-roller melt spinning at lower substrate velocities (Vs, 8–15 m/s). The degree of preferred orientation (DPO) of spun flakes calculated from x-ray diffraction patterns is 70%–97% on the free surface, 50%–80% on the wheel surface, at Vs=8, 10 m/s. In the case of adding 1 at. % of Ti/V/Mo/Zr/Ta, Vs=8 m/s, the resultant DPO value can be higher than 50% across the whole thickness. Magnetic measurements on spun flakes show highly anisotropic behavior. Maximum energy product of Nd13Fe80ZrB6 flakes spun at 12 m/s, pulse magnetized to 5.5 T, and measured normal or parallel to the flake surface is 144 kJ/m3 (18 MGOe) or 124 kJ/m3 (15.5 MGOe), respectively. |
doi_str_mv | 10.1063/1.106127 |
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H ; YAU, J. M</creator><creatorcontrib>TSUNG-SHUNE CHIN ; HUANG, S. H ; YAU, J. M</creatorcontrib><description>Anisotropic Nd13Fe81−xMxB6 flakes (M=0.5–3 at. % one of Ti/Zr/V/Ta/Mo/Zn) are reproducibly obtainable using single-roller melt spinning at lower substrate velocities (Vs, 8–15 m/s). The degree of preferred orientation (DPO) of spun flakes calculated from x-ray diffraction patterns is 70%–97% on the free surface, 50%–80% on the wheel surface, at Vs=8, 10 m/s. In the case of adding 1 at. % of Ti/V/Mo/Zr/Ta, Vs=8 m/s, the resultant DPO value can be higher than 50% across the whole thickness. Magnetic measurements on spun flakes show highly anisotropic behavior. Maximum energy product of Nd13Fe80ZrB6 flakes spun at 12 m/s, pulse magnetized to 5.5 T, and measured normal or parallel to the flake surface is 144 kJ/m3 (18 MGOe) or 124 kJ/m3 (15.5 MGOe), respectively.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.106127</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>Melville, NY: American Institute of Physics</publisher><subject>Applied sciences ; Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Exact sciences and technology ; Magnetic anisotropy ; Magnetic properties and materials ; Magnetically ordered materials: other intrinsic properties ; Metals. 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M</creatorcontrib><title>Anisotropic Nd-Fe-M-B flakes by single-roller melt spinning</title><title>Applied physics letters</title><description>Anisotropic Nd13Fe81−xMxB6 flakes (M=0.5–3 at. % one of Ti/Zr/V/Ta/Mo/Zn) are reproducibly obtainable using single-roller melt spinning at lower substrate velocities (Vs, 8–15 m/s). The degree of preferred orientation (DPO) of spun flakes calculated from x-ray diffraction patterns is 70%–97% on the free surface, 50%–80% on the wheel surface, at Vs=8, 10 m/s. In the case of adding 1 at. % of Ti/V/Mo/Zr/Ta, Vs=8 m/s, the resultant DPO value can be higher than 50% across the whole thickness. Magnetic measurements on spun flakes show highly anisotropic behavior. Maximum energy product of Nd13Fe80ZrB6 flakes spun at 12 m/s, pulse magnetized to 5.5 T, and measured normal or parallel to the flake surface is 144 kJ/m3 (18 MGOe) or 124 kJ/m3 (15.5 MGOe), respectively.</description><subject>Applied sciences</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Exact sciences and technology</subject><subject>Magnetic anisotropy</subject><subject>Magnetic properties and materials</subject><subject>Magnetically ordered materials: other intrinsic properties</subject><subject>Metals. Metallurgy</subject><subject>Physics</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1991</creationdate><recordtype>article</recordtype><recordid>eNo9kEFLAzEUhIMoWKvgT9iDiJfoe8lms8FTLVaFqhc9hzSbSDTdXZPtof_eLS2ehhk-hmEIuUS4Raj4He4EmTwiEwQpKUesj8kEADitlMBTcpbz92gF43xC7mdtyN2Quj7Y4q2hC0df6UPho_lxuVhtixzar-ho6mJ0qVi7OBS5D207xufkxJuY3cVBp-Rz8fgxf6bL96eX-WxJLavFQL1pQDLrmso4YwDKlWkqVKpUzPEVMKgYK430gnPBBEpXg6isKcEjcKY8n5LrfW-fut-Ny4Neh2xdjKZ13SZrJniJiqkRvNmDNnU5J-d1n8LapK1G0Lt3NOr9OyN6deg02Zrok2ltyP_8OEPWiPwPli1hDw</recordid><startdate>19911014</startdate><enddate>19911014</enddate><creator>TSUNG-SHUNE CHIN</creator><creator>HUANG, S. H</creator><creator>YAU, J. M</creator><general>American Institute of Physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>19911014</creationdate><title>Anisotropic Nd-Fe-M-B flakes by single-roller melt spinning</title><author>TSUNG-SHUNE CHIN ; HUANG, S. H ; YAU, J. M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c285t-fad072ced6aeaa004bad6199492e3b0206224a7f53352517e8056ca40f10329f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1991</creationdate><topic>Applied sciences</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Exact sciences and technology</topic><topic>Magnetic anisotropy</topic><topic>Magnetic properties and materials</topic><topic>Magnetically ordered materials: other intrinsic properties</topic><topic>Metals. Metallurgy</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>TSUNG-SHUNE CHIN</creatorcontrib><creatorcontrib>HUANG, S. H</creatorcontrib><creatorcontrib>YAU, J. M</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>TSUNG-SHUNE CHIN</au><au>HUANG, S. H</au><au>YAU, J. M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Anisotropic Nd-Fe-M-B flakes by single-roller melt spinning</atitle><jtitle>Applied physics letters</jtitle><date>1991-10-14</date><risdate>1991</risdate><volume>59</volume><issue>16</issue><spage>2046</spage><epage>2048</epage><pages>2046-2048</pages><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>Anisotropic Nd13Fe81−xMxB6 flakes (M=0.5–3 at. % one of Ti/Zr/V/Ta/Mo/Zn) are reproducibly obtainable using single-roller melt spinning at lower substrate velocities (Vs, 8–15 m/s). The degree of preferred orientation (DPO) of spun flakes calculated from x-ray diffraction patterns is 70%–97% on the free surface, 50%–80% on the wheel surface, at Vs=8, 10 m/s. In the case of adding 1 at. % of Ti/V/Mo/Zr/Ta, Vs=8 m/s, the resultant DPO value can be higher than 50% across the whole thickness. Magnetic measurements on spun flakes show highly anisotropic behavior. Maximum energy product of Nd13Fe80ZrB6 flakes spun at 12 m/s, pulse magnetized to 5.5 T, and measured normal or parallel to the flake surface is 144 kJ/m3 (18 MGOe) or 124 kJ/m3 (15.5 MGOe), respectively.</abstract><cop>Melville, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.106127</doi><tpages>3</tpages></addata></record> |
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subjects | Applied sciences Condensed matter: electronic structure, electrical, magnetic, and optical properties Exact sciences and technology Magnetic anisotropy Magnetic properties and materials Magnetically ordered materials: other intrinsic properties Metals. Metallurgy Physics |
title | Anisotropic Nd-Fe-M-B flakes by single-roller melt spinning |
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