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Micromagnetic simulations of spinel ferrite particles

机译:尖晶石铁氧体颗粒的微磁模拟

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摘要

This paper presents the results of simulations of the magnetization field{\it ac} response (at $2$ to $12$ GHz) of various submicron ferrite particles(cylindrical dots). The ferrites in the present simulations have the spinelstructure, expressed here by M$_{1-n}$Zn$_{n}$Fe$_2$O$_4$ (where M stands for adivalent metal), and the parameters chosen were the following: (a) for $n=0$: M= \{ Fe, Mn, Co, Ni, Mg, Cu \}; (b) for $n=0.1$: M = \{ Fe, Mg \} (mixedferrites). These runs represent full 3D micromagnetic (one-particle) ferritesimulations. We find evidences of confined spin waves in all simulations, aswell as a complex behavior nearby the main resonance peak in the case of the M= \{ Mg, Cu \} ferrites. A comparison of the $n=0$ and $n=0.1$ cases for fixedM reveals a significant change in the spectra in M = Mg ferrites, but only aminor change in the M = Fe case. An additional larger scale simulation of a $3$by $3$ particle array was performed using similar conditions of the Fe$_3$O$_4$(magnetite; $n=0$, M = Fe) one-particle simulation. We find that the mainresonance peak of the Fe$_3$O$_4$ one-particle simulation is disfigured in thecorresponding 3 by 3 particle simulation, indicating the extent to whichdipolar interactions are able to affect the main resonance peak in thatmagnetic compound.
机译:本文介绍了各种亚微米铁氧体颗粒(圆柱点)的磁化场响应(在2美元至12美元GHz时)的仿真结果。本模拟中的铁氧体具有尖晶石结构,在此表示为M $ _ {1-n} $ Zn $ _ {n} $ Fe $ _2 $ O $ _4 $(其中M代表价金属),并选择了参数以下是:(a)对于$ n = 0 $:M = \ {铁,锰,钴,镍,镁,铜\}; (b)对于$ n = 0.1 $:M = \ {Fe,Mg \}(混合铁氧体)。这些运行代表完整的3D微磁(单粒子)铁氧体模拟。我们在所有模拟中都发现了自旋波受限的证据,并且在M = \ {Mg,Cu \}铁氧体的情况下,还发现了主共振峰附近的复杂行为。对fixedM的$ n = 0 $和$ n = 0.1 $情况的比较显示M = Mg铁氧体的光谱有显着变化,但在M = Fe情况下只有氨基变化。使用Fe $ _3 $ O $ _4 $(磁铁矿; $ n = 0 $,M = Fe)单粒子模拟的类似条件对$ 3 $ * $ 3 $粒子阵列进行了更大范围的模拟。我们发现,Fe $ _3 $ O $ _4 $单粒子模拟的主共振峰在相应的3×3粒子模拟中被毁坏,表明偶极相互作用能够影响该磁性化合物中主共振峰的程度。

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