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Rare-earth intermetallics such as Nd2FeI4B and Sm-Co are widely used as high-performance permanent magnets,because they combine high magnetocrystalline anisotropy with reasonable magnetization and Curie temperature.The anisotropy is a combined effect of spin-orbit coupling and electrostatic crystal-field interactions.The main contribution comes from the rare-earth 4f electrons,which are well-screened from the crystalline environment but exhibit a strong spin-orbit coupling.In this limit,the magnetocrystalline anisotropy has a very transparent physical interpretation,the anisotropy energy essentially being equal to the energy of Hund's-rules 4f ion in the crystal field.The corresponding expression for the lowest-order uniaxial anisotropy constant K1 is used to discuss rare-earth substitutions,which have recently attracted renewed interest due to shifts in the rare-earth production and demand.Specific phenomena reviewed in this article are the enhancement of the anisotropy of Sm2Fe17 due to interstitial nitrogen,the use of Sm-Co magnets for high-temperature applications,and the comparison of rare-earth single-ion anisotropy with other single-ion and two-ion mechanisms.

参考文献

[1] Kumar K .RETM5 and RE2TM17 permanent magnets development[J].Journal of Applied Physics,1988,63:R13.
[2] Sagawa M;Fujimura S;Yamamoto H;Matsuura Y .Permanent magnet materials based on the rare earth-iron-boron tetragonal compounds[J].IEEE Transactions on Magnetics,1984,20(05):1584.
[3] Herbst J F .R2Fe14B materials:Intrinsic properties and technological aspects[J].Reviews of Modern Physics,1991,63:819.
[4] Skomski R;Coey J M D.Permanent Magnetism[M].Bristol:Institute of Physics,1999
[5] Coey J M D;Sun H .Improved magnetic properties by treatment iron-based rare-earth intermetallic compounds in ammonia[J].Journal of Magnetism and Magnetic Materials,1990,87:L251.
[6] Coey J M D .Rare-earth Iron Permanent Magnets[D].Oxford:University Press,1996.
[7] Bloch F;Gentile G .Zur Anisotropie der Magnetisierung ferromagnetischer Einkristalle[J].Z Phys,1931,70:395.
[8] Skomski R .Simple Models of Magnetism[D].Oxford:University Press,2008.
[9] Abragam A;Bleaney B .Electron Paramagnetic Resonance of Transition Ions[D].Oxford:University Press,1970.
[10] C Rudowicz .Concept of spin Hamiltonian,forms of zero field splitting and electronic Zeeman Hamiltonians and relations between parameters used in EPR.A critical review[J].Magn Reson Rev,1987,13:1.
[11] Newman D J;Ng B .The superposition model of crystal fields[J].Reports on Progress in Physics,1989,52:699.
[12] Rudowicz Cz .On the derivation of the superposition model formulas using the transformation relations for the Stevens operators[J].J Phys C,1987,20:6033.
[13] Akulov N .Zur quantentheorie der temperaturabhangigkeit der magnefisierungskurve[J].Z Phys,1936,100:197.
[14] Callen E R .Texture dependence of ferromagnetic uniaxial anisotropy constants[J].Journal of Applied Physics,1962,33:832.
[15] Callen H R;Callen E .The present status of the temperature dependence of the magnetocrystalline anisotropy and the 1(1+1) power law[J].Journal of Physics and Chemistry of Solids,1966,27:1271.
[16] Skomski R;Mryasov ON;Zhou J;Sellmyer DJ .Finite-temperature anisotropy of magnetic alloys[J].Journal of Applied Physics,2006(8):E8916-1-E8916-3-0.
[17] Staunton J B;Ostanin S;Razee S S A;Gyorffy B L Szunyogh L Ginatempo B Bruno E .Temperature dependent magnetic anisotropy in metallic magnets from an ab-initio electronic structure theory:L10-ordered FePt[J].Physical Review Letters,2004,93:257204-2571-4.
[18] Skomski R;Kashyap A;Sellmyer D J .Finite-temperature Anisotropy of PtCo Magnets[J].IEEE Transactions on Magnetics,2003,39:2917.
[19] Zhou J;Skomski R;Chela C;Hadjipanayis G C Sellmyer D J .Sm-Co-Ti high-temperature permanent magnets[J].Applied Physics Letters,2000,77:1514.
[20] Skomski R .The screened-charge model of crystal-field interaction[J].Phil,Mag B,1994,70:175.
[21] Ballhausen C J.Ligand Field Theory[M].New York:McGraw-Hill,1962
[22] Schrnitt D .Contribution of the conduction electrons to the crystalline electric field.I:direct coulombic part[J].J Phys F,1979,9:1745.
[23] Schmitt D .Contribution of the conduction electrons to the crystalline electric field.Ⅱ:exchange coulombic Part[J].J Phys F,1979,9:1759.
[24] Neel L .Anisotropie magnetique superficielle et surstructures d'Orientation,J[J].Phys Radium,1954,15:225.
[25] Skomski R.;Jaswal SS.;Sabiryanov RF. .Ruderman-Kittel-Kasuya-Yosida interactions between spin distributions of arbitrary shape[J].Journal of Applied Physics,2000(9 Pt.2):5890-5892.
[26] Haskel D;Lang JC;Islam Z;Cady A;Srajer G;van Veenendaal M;Canfield PC .Atomic origin of magnetocrystalline anisotropy in Nd2Fe14B[J].Physical review letters,2005(21):7207-1-7207-4-0.
[27] Kuz'min M D .Comment[J].Physical Review Letters,2006,97:259701-2591-1.
[28] Sellmyer D J;Skomski R.Advanced Magnetic Nanostructures[M].Berlin:springer-verlag,2006
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