Increase in Nucleation Field of Nanocrystalline Nd(Fe,Co)B Magnets Due to Strengthening of Exchange Interaction-Computer Simulation

The effect of the strength of exchange interaction on the nucleation field H_{N} was studied by computer simulation with varying temperature as well as the size of the non-magnetic phase for Nd(Fe,Co)B magnets composed of fine grains. It was clarified that the spatial distribution of demagnetizing...

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Veröffentlicht in:IEEE transactions on magnetics 2018-11, Vol.54 (11), p.1-5
Hauptverfasser: Fukunaga, H., Harada, T., Yanai, T., Nakano, M.
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Harada, T.
Yanai, T.
Nakano, M.
description The effect of the strength of exchange interaction on the nucleation field H_{N} was studied by computer simulation with varying temperature as well as the size of the non-magnetic phase for Nd(Fe,Co)B magnets composed of fine grains. It was clarified that the spatial distribution of demagnetizing field H_{d} is widened by an increase in the size of the non-magnetic phase and that the ratio of the spatial size of H_{d} to the exchange length L_{\mathrm {ex}} is an important factor of determining H_{N} . Resultantly, the increase in the exchange strength increased H_{N} . Based on this calculation result, magnetic properties of Nd(Fe,Co)B magnets were simulated and it was found that a small amount of substitution of Co for Fe increases L_{\mathrm {ex}} and resultantly improves H_{N} at high temperatures.
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It was clarified that the spatial distribution of demagnetizing field <inline-formula> <tex-math notation="LaTeX">H_{d} </tex-math></inline-formula> is widened by an increase in the size of the non-magnetic phase and that the ratio of the spatial size of <inline-formula> <tex-math notation="LaTeX">H_{d} </tex-math></inline-formula> to the exchange length <inline-formula> <tex-math notation="LaTeX">L_{\mathrm {ex}} </tex-math></inline-formula> is an important factor of determining <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula>. Resultantly, the increase in the exchange strength increased <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula>. Based on this calculation result, magnetic properties of Nd(Fe,Co)B magnets were simulated and it was found that a small amount of substitution of Co for Fe increases <inline-formula> <tex-math notation="LaTeX">L_{\mathrm {ex}} </tex-math></inline-formula> and resultantly improves <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula> at high temperatures.]]></description><identifier>ISSN: 0018-9464</identifier><identifier>EISSN: 1941-0069</identifier><identifier>DOI: 10.1109/TMAG.2018.2846703</identifier><identifier>CODEN: IEMGAQ</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Cobalt ; Computational modeling ; Computer simulation ; Demagnetization ; Demagnetization field ; Elementary particle exchange interactions ; exchange length ; Exchanging ; Iron ; Magnetic properties ; Magnetism ; Magnetization ; Magnets ; micromagnetics simulation ; Nd–Fe–B ; Neodymium ; Nucleation ; Perpendicular magnetic anisotropy ; Spatial distribution ; Temperature dependence</subject><ispartof>IEEE transactions on magnetics, 2018-11, Vol.54 (11), p.1-5</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. 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It was clarified that the spatial distribution of demagnetizing field <inline-formula> <tex-math notation="LaTeX">H_{d} </tex-math></inline-formula> is widened by an increase in the size of the non-magnetic phase and that the ratio of the spatial size of <inline-formula> <tex-math notation="LaTeX">H_{d} </tex-math></inline-formula> to the exchange length <inline-formula> <tex-math notation="LaTeX">L_{\mathrm {ex}} </tex-math></inline-formula> is an important factor of determining <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula>. Resultantly, the increase in the exchange strength increased <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula>. Based on this calculation result, magnetic properties of Nd(Fe,Co)B magnets were simulated and it was found that a small amount of substitution of Co for Fe increases <inline-formula> <tex-math notation="LaTeX">L_{\mathrm {ex}} </tex-math></inline-formula> and resultantly improves <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula> at high temperatures.]]></description><subject>Cobalt</subject><subject>Computational modeling</subject><subject>Computer simulation</subject><subject>Demagnetization</subject><subject>Demagnetization field</subject><subject>Elementary particle exchange interactions</subject><subject>exchange length</subject><subject>Exchanging</subject><subject>Iron</subject><subject>Magnetic properties</subject><subject>Magnetism</subject><subject>Magnetization</subject><subject>Magnets</subject><subject>micromagnetics simulation</subject><subject>Nd–Fe–B</subject><subject>Neodymium</subject><subject>Nucleation</subject><subject>Perpendicular magnetic anisotropy</subject><subject>Spatial distribution</subject><subject>Temperature dependence</subject><issn>0018-9464</issn><issn>1941-0069</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNo9kE1LwzAYx4MoOF8-gHgJeFGwM0mTtjnq3HSwzcN2L2n6tFa6ZCYpuLNf3NaJp4c_z_8FfghdUTKmlMiHzfLxZcwIzcYs40lK4iM0opLTiJBEHqMR6V-R5Ak_RWfef_SSC0pG6HtutAPlATcGrzrdggqNNXjWQFtiW-GVMla7vQ-qbRsDeFXezuB-Yu-e8FLVBoLHzx3gYPE6ODB1eAfTmHqITr_0uzI14LkJ4JQeiqOJ3e66XuJ1s-3a37ELdFKp1sPl3z1Hm9l0M3mNFm8v88njItKMixBpIARIkVaSqTLTVaVinnIAIaqiUElKZcKZKDVPhCw5LxSXkJQZJVwJLWR8jm4OtTtnPzvwIf-wnTP9Ys4oozJOpUx7Fz24tLPeO6jynWu2yu1zSvIBdT6gzgfU-R_qPnN9yDQA8O_POGFM8PgH0BV7vA</recordid><startdate>20181101</startdate><enddate>20181101</enddate><creator>Fukunaga, H.</creator><creator>Harada, T.</creator><creator>Yanai, T.</creator><creator>Nakano, M.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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It was clarified that the spatial distribution of demagnetizing field <inline-formula> <tex-math notation="LaTeX">H_{d} </tex-math></inline-formula> is widened by an increase in the size of the non-magnetic phase and that the ratio of the spatial size of <inline-formula> <tex-math notation="LaTeX">H_{d} </tex-math></inline-formula> to the exchange length <inline-formula> <tex-math notation="LaTeX">L_{\mathrm {ex}} </tex-math></inline-formula> is an important factor of determining <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula>. Resultantly, the increase in the exchange strength increased <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula>. Based on this calculation result, magnetic properties of Nd(Fe,Co)B magnets were simulated and it was found that a small amount of substitution of Co for Fe increases <inline-formula> <tex-math notation="LaTeX">L_{\mathrm {ex}} </tex-math></inline-formula> and resultantly improves <inline-formula> <tex-math notation="LaTeX">H_{N} </tex-math></inline-formula> at high temperatures.]]></abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TMAG.2018.2846703</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0002-7990-3370</orcidid></addata></record>
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subjects Cobalt
Computational modeling
Computer simulation
Demagnetization
Demagnetization field
Elementary particle exchange interactions
exchange length
Exchanging
Iron
Magnetic properties
Magnetism
Magnetization
Magnets
micromagnetics simulation
Nd–Fe–B
Neodymium
Nucleation
Perpendicular magnetic anisotropy
Spatial distribution
Temperature dependence
title Increase in Nucleation Field of Nanocrystalline Nd(Fe,Co)B Magnets Due to Strengthening of Exchange Interaction-Computer Simulation
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