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复合外场中磁光材料(BiTm)3(FeGa)5O12薄膜畴壁运动特性的研究
引用本文:曾文光,邓雪儿,程玮,吴木营,林长净,冯稷.复合外场中磁光材料(BiTm)3(FeGa)5O12薄膜畴壁运动特性的研究[J].发光学报,2001,22(2):103-106.
作者姓名:曾文光  邓雪儿  程玮  吴木营  林长净  冯稷
作者单位:1. 东莞理工学院计算机系, 广东东莞 511700;2. 香港城市大学物理与材料科学系
摘    要:通过对BiTm)3(FeGa)5O12膜施工加低频交变磁场,匀速率增加的直流磁场和同时对该膜施加这两种磁场(复合外场),用照相划线读数方法和通过电荷耦合器件(CCD)-计算机作数字化处理获得磁畴壁(DW)的相对百分数。结果表明:(1)复合外场下DW运动规律中存在交互作用项;(2)低频交变磁场幅值(140A/m)远低于等效阻力场(103A/m)时,DW可以运动,但不同步,频率大于1Hz时明显滞后,(3)利用图像转换有利于提高实验结果的分辨率。

关 键 词:磁光膜  畸壁运动  相互作用
文章编号:1000-7032(2001)02-0103-04
收稿时间:2000-08-11
修稿时间:2000年8月11日

Dynamic Behavior of Magnetic Domain Walls in (BiTm)3-(FeGa)5O12 Thin Film under the Composite Field
ZENG Wen-guang,DENG Xue-er,LIN Chang-jing,FENG Ji,CHENG Wei,WU Mu-ying.Dynamic Behavior of Magnetic Domain Walls in (BiTm)3-(FeGa)5O12 Thin Film under the Composite Field[J].Chinese Journal of Luminescence,2001,22(2):103-106.
Authors:ZENG Wen-guang  DENG Xue-er  LIN Chang-jing  FENG Ji  CHENG Wei  WU Mu-ying
Institution:1. Dongguan Institute of Technology, Guangdong Dongguan 511700, China;2. City University of Hong Kong, Hong Kong, China
Abstract:The motion characteristics of the magnetic thin film have been studied under various forms of applied magnetic field(AMF):pulse,A.C. field and D.C.field 1~6].In present paper,the dynamic behaviour of the magntooptic thin film under the composite fields has been measured experimentally.The formula of magnetooptic specimen is BiTm)3(FeGa)5O12,which has two surface with thickness of 6 19×2μm.The AMF corresponding the saturation Faraday's rotation angle is 8000A/m.The domain wall(DW) can be considered as the 180 degree wall and the equivalent resistant field is the order of 1000A/m in the thin film specimen.There are three forms of AMF:type A,low frequency A.C.(the amplitude 140A/m) produced by a function generator;type B,uniform magnetic field sweeping(UMFS,d H/dt=83.6A/m/S in present paper,H is the magnetic field) produced by a D.C. power supply with a sweeping rate control system 6];type C,the UMFS together with low frequency A.C.field.We remark the type C as the composite field.The data of DWs motion have been obtained by means of the computer with charge couple device(CCD) and of photography from the polarization microscope.The transformer put on the stage of the microscope was prepared a fair hole to lay up the thin film specimen and was connected to the D.C.power supply or/and to the function generator for carrying out AMF.The average distance of DWs from the photography for various experiment conditions of H could be plotted against the time.The percentage data of DWs area from the CCD for various experiment conditions of H do the time in the same grapher.After comparing the dynamic character of DWs with these curves corresponding to 0.1~10Hz A.C.fields or/and to H/dt=83.6A/m/S UMFS rate,it can be shown that: (1)The motion behaviors of DWs in the AMF of type C are not the same as that of simple composition of type A and type B,it would be an interaction term represented the force between AMF and DWs 7].(2)Even if the amplitude of A.C.field value 140A/m1000A/m,the equivalent resistant field 6],and the value of D.C.field100A/m,the DWs of the thin film specimen can be moved.The motion of DWs is not synchronized with the AMF.It is supposed that the DWs may be easier to move and can be pushed forward or pulled back by a small D.C.field superposed a weak A.C.field.
Keywords:magnetic thin film  domain wall motion  interaction
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