3D and 1D micromagnetic calculation for hard/soft bilayers with in-plane easy axes

被引:36
|
作者
Zhang, Wei [1 ]
Zhao, G. P. [1 ,2 ]
Yuan, X. H. [1 ]
Ye, L. N. [3 ]
机构
[1] Sichuan Normal Univ, Coll Phys & Elect Engn, Chengdu 610066, Peoples R China
[2] Univ Elect Sci & Technol China, State Key Lab Elect Thin Films & Integrated Devic, Chengdu 610054, Peoples R China
[3] SW Univ Finance & Econ, Sch Econ Informat Engn, Chengdu 610074, Peoples R China
基金
中国国家自然科学基金;
关键词
Hard/soft bilayer; Hysteresis loop; Micromagnetic calculation; REMANENCE ENHANCEMENT; MAGNETS; NANOLAYERS;
D O I
10.1016/j.jmmm.2012.07.053
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Macroscopic hysteresis loops and microscopic magnetic moment distributions have been determined by three-dimensional (3D) as well as one-dimensional (1D) micromagnetic models for exchange coupled Nd2Fe14B/alpha-Fe bilayers and carefully compared with each other. It is found that the results obtained from the two methods are consistent with each other, where the nucleation and coercive fields decrease monotonically as the soft layer thickness L-s increases whilst the largest maximum energy products (roughly 600 kJ/m(3)) occur at L-s = 5 nm. Moreover, the calculated angular distributions in the thickness direction for the magnetic moments are similar. Nevertheless, the calculated critical fields and energy products by 3D OOMMF are systematically smaller than those given by the 1D model, mainly due to the local demagnetization fields, which are taken into account in the 3D calculation and ignored in the 1D calculation. It is demonstrated by the 3D calculation that the large demagnetization fields in the corners of the soft layers reduce the nucleation fields and thus facilitate the magnetic reversal. Such an effect enhancesas L-s increases. When L-s=20 nm, the differences between the coercivity is as large as 30%, while the nucleation fields obtained by the two methods have opposite signs. (c) 2012 Elsevier B.V. All rights reserved.
引用
收藏
页码:4231 / 4236
页数:6
相关论文
共 50 条
  • [41] GPU efficient 1D and 3D recursive filtering
    Maximo, Andre
    DIGITAL SIGNAL PROCESSING, 2021, 114
  • [42] Reducing 3D Vibrations to 1D in Real Time
    Park, Gunhyuk
    Kuchenbecker, Katherine J.
    HAPTIC INTERACTION: PERCEPTION, DEVICES AND ALGORITHMS, 2019, 535 : 21 - 24
  • [43] 3D reconstruction algorithm based on 1D subspace
    Liu, Shi-Gang
    Peng, Ya-Li
    Han, Chong-Zhao
    Wang, Ying-Hua
    Jiqiren/Robot, 2009, 31 (03): : 224 - 228
  • [44] Simulations of the ripening of 3D, 2D and 1D objects
    Bonafos, C
    Colombeau, B
    Carrada, M
    Altibelli, A
    Claverie, A
    MATERIALS SCIENCE AND ENGINEERING B-SOLID STATE MATERIALS FOR ADVANCED TECHNOLOGY, 2002, 88 (2-3): : 112 - 117
  • [45] Synthesis of 1D, 2D, and 3D structures of phosphorus
    Ji, Haifeng
    Smith, Joshua
    Hagaman, Daniel
    ABSTRACTS OF PAPERS OF THE AMERICAN CHEMICAL SOCIETY, 2016, 252
  • [47] 3D and 1D calculation of hysteresis loops and energy products for anisotropic nanocomposite films with perpendicular anisotropy
    Yuan, X. H.
    Zhao, G. P.
    Yue, Ming
    Ye, L. N.
    Xia, J.
    Zhang, X. C.
    Chang, J.
    JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, 2013, 343 : 245 - 250
  • [48] Inductance calculation of 3D superconducting structures with ground plane
    Teh, CK
    Kitagawa, M
    Okabe, Y
    SUPERCONDUCTOR SCIENCE & TECHNOLOGY, 1999, 12 (11): : 921 - 924
  • [49] 3D printed NMR spectra: From 1D and 2D acquisition to 3D visualization
    Bakker, Michael
    Boyd, Ben
    Meints, Gary A.
    CONCEPTS IN MAGNETIC RESONANCE PART A, 2018, 47A (01)
  • [50] In-plane and out-of-plane characterization of a 3D angle interlock textile composite
    Dau, F.
    Dano, M-L
    Verone, B.
    Girardot, J.
    Aboura, Z.
    Morvan, J-M
    COMPOSITES PART A-APPLIED SCIENCE AND MANUFACTURING, 2021, 149