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采用射频(RF)磁控溅射方法,在2种基底温度(TS =25,310℃)的基片上制备了结构为Si(111)/NdFeCo(610 nm)/Cr(10 nm)的薄膜样品,溅射氩气压保持在pAr=0.1 Pa.采用X射线衍射仪(XRD)、场发射扫描电镜(FE-SEM)、振动样品磁强计(VSM)、原子力显微镜(AFM)和磁力显微镜(MFM)等实验技术,研究了一步和三步快速退火(RTA-Ⅰ和RTA-Ⅱ)工艺对两种薄膜微结构和磁性的影响.结果显示,室温基底上沉积的样品呈非晶态,磁畴为面内磁畴结构;而加热基底上制备的样品则析出了Nd2 Fe17和Nd6 Fe13 Si纳米晶,垂直磁各向异性(PMA)反常增强,垂直磁各向异性能为K⊥=1.18×105 J·m-3,磁畴为平行条纹畴.在TA =500℃经过RTA-Ⅰ/-Ⅱ工艺后,基底加热样品析出的Nd2 Fe17和Nd6Fe13Si纳米晶继续长大,磁畴由条纹畴转变为磁斑畴.而室温基底上制备的薄膜经RTA-Ⅰ/-Ⅱ退火后则没有观察到界面硅化物,却发现结晶出的FeCo和Nd2 Fe15 Co2纳米晶粒大小和取向敏感地依赖于退火工艺.即一步快速退火工艺有利于析出(111)织构的Nd2 Fe15 Co2纳米晶,而三步快速退火工艺则易于诱导出(200)织构的FeCo纳米晶.实验结果表明,基底加热薄膜中析出的Nd2 Fe17纳米晶与Nd6 Fe13 Si界面硅化物的热膨胀特性正好相反,由此产生的残余内应力与磁弹各向异性,是导致基底加热薄膜PMA反常增强的主要原因.

参考文献

[1] Ohmori H;Hatori T;Nakagawa S .Perpendicular magnetic tunnel junction with tunneling magnetoresistance ratio of 64% using MgO (100) barrier layer prepared at room temperature[J].Journal of Applied Physics,2008(7 Pt.2):A7911-1-A7911-3-0.
[2] 刘娜,王海,朱涛.CoFeB/Pt多层膜的垂直磁各向异性研究[J].物理学报,2012(16):443-446.
[3] 刘帅,俱海浪,于广华,李宝河,陈晓白.Co/Pt多层膜反常霍尔效应的研究[J].稀有金属,2014(05):762-767.
[4] Harris VG.;Pokhil T. .Selective-resputtering-induced perpendicular magnetic anisotropy in amorphous TbFe films - art. no. 067207[J].Physical review letters,2001(6):7207-0.
[5] Zhang, WY;Shima, H;Takano, F;Takenaka, M;Yamazaki, M;Masuda, K;Akinaga, H;Nagahama, T;Nimori, S .Origin of perpendicular magnetic anisotropy and evolution of magnetic domain structure of amorphous Pr-TM-B (TM=Fe, Co) films[J].Journal of Magnetism and Magnetic Materials,2010(8):900-908.
[6] Xi, L;Lu, JM;Zhou, JJ;Sun, QJ;Xue, DS;Li, FS .Thickness dependence of magnetic anisotropic properties of FeCoNd films[J].Journal of Magnetism and Magnetic Materials,2010(15):2272-2275.
[7] Youxing Yu;Youran Yang;Yijiao Shan;Xiaofang Bi .Abnormal substrate temperature dependent out-of-plane anisotropy in FeCoNbB amorphous films[J].Applied physics letters,2012(23):232408-1-232408-4.
[8] Anjum, S.;Rafique, M.S.;Khaleeq-Ur-Rahman, M.;Siraj, K.;Usman, A.;Latif, H.;Bhatti, K.A.;Hussain, S.;Naseem, S. .Magnetic and optical properties of amorphous NdFeCo thin films by pulsed laser deposition technique[J].Vacuum: Technology Applications & Ion Physics: The International Journal & Abstracting Service for Vacuum Science & Technology,2010(2):126-130.
[9] Sharma P;Kimura H;Inoue A;Arenholz E;Guo JH .Temperature and thickness driven spin-reorientation transition in amorphous Co-Fe-Ta-B thin films[J].Physical review, B. Condensed matter and materials physics,2006(5):2401-1-2401-4-0.
[10] Alvarez-Prado LM.;Alameda JM. .Micromagnetism of nanowires with low out-of plane-anisotropy[J].Physica, B. Condensed Matter,2004(1/4):241-246.
[11] P. Iranmanesh;N. Tajabor;M. Rezaee Roknabadi .Influence of Co substitution on magnetic properties and thermal expansion of Nd_6Fe_(13)Si intermetallic compound[J].Intermetallics,2011(5):682-687.
[12] A.L. Xia;H.L. Zhang;L.N. Tong;B.S. Han .Lattice mismatch induced weak perpendicular anisotropy in Fe/Co multilayers prepared by direct current magnetron sputtering[J].Thin Solid Films: An International Journal on the Science and Technology of Thin and Thick Films,2008(21):7653-7656.
[13] Arnold Z.;Morellon L.;Ibarra MR.;Kamarad J. .MAGNETOVOLUME EFFECTS AND ANOMALOUS COMPRESSIBILITY OF ND2FE17 AND ND-2(FETI)(17) COMPOUNDS[J].Journal of Applied Physics,1997(8 Pt.2b):5693-5695.
[14] Shen BG.;Cheng ZH.;Gong HY.;Zhan WS.;Tang H.;Deboer FR. Buschow JHJ.;Liang B. .MAGNETIC PROPERTIES OF R2FE14M3 COMPOUNDS WITH M=GA AND SI R=Y, ND, SM, GD, TB, DY, HO, ER AND TM[J].Solid State Communications,1997(2):71-75.
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