Probing dynamical magnetization pinning in circular dots as a function of the external magnetic field orientation

被引:19
|
作者
Kakazei, G. N. [1 ,2 ]
Aranda, G. R. [3 ]
Bunyaev, S. A. [1 ,2 ]
Golub, V. O. [4 ]
Tartakovskaya, E. V. [4 ]
Chumak, A. V. [5 ,7 ]
Serga, A. A. [5 ,7 ]
Hillebrands, B. [5 ,7 ]
Guslienko, K. Y. [3 ,6 ]
机构
[1] Univ Porto, IFIMUP IN Inst Nanosci & Nanotechnol, P-4169007 Oporto, Portugal
[2] Univ Porto, Dept Fis, P-4169007 Oporto, Portugal
[3] Univ Pais Vasco UPV EHU, Dept Fis Mat, San Sebastian 20018, Spain
[4] Natl Acad Sci Ukraine, Inst Magnetism, UA-03142 Kiev, Ukraine
[5] Tech Univ Kaiserslautern, Fachbereich Phys, D-67663 Kaiserslautern, Germany
[6] Basque Fdn Sci, IKERBASQUE, Bilbao 48011, Spain
[7] Tech Univ Kaiserslautern, Forschungszentrum OPTIMAS, D-67663 Kaiserslautern, Germany
来源
PHYSICAL REVIEW B | 2012年 / 86卷 / 05期
关键词
SPIN-WAVE RESONANCE; FERROMAGNETIC-RESONANCE; ARRAYS; MODES; ANISOTROPIES; INPLANE; FILMS;
D O I
10.1103/PhysRevB.86.054419
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We performed ferromagnetic resonance measurements of square arrays of noninteracting Permalloy circular dots for different orientations of external magnetic field with respect to the patterned film plane (theta). Out-of-plane angular dependence of the main resonance peak was measured in the whole range of the field angles 0 degrees <= theta <= 90 degrees. The main eigenmodespatial distribution is strongly nonuniform due to the dot nonellipsoidal shape. Nevertheless, for dots with small aspect ratio b = L/R <= 0.1 (where R is dot radius and L is dot thickness) Kittel's equation, assuming uniform dynamic magnetization (no pinning at the dot lateral edges), describes the peak position with high accuracy. Analytical calculations and micromagnetic simulations confirmed the gradual evolution of the main mode profile and a smooth transition from the strong to relatively weak pinning conditions with the change of external magnetic field angle.
引用
收藏
页数:7
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