电流调控磁涡旋的极性和旋性

提出了一种特殊自旋阀结构, 其极化层(钉扎层)磁矩沿面内方向, 自由层磁矩成磁涡旋结构. 自由层在形状上设计成左右两边厚度不同的阶梯形圆盘. 微磁学模拟研究发现, 通过调控所施加的高斯型脉冲电流的大小、方向和脉冲宽度, 可以实现磁涡旋的不同旋性、不同极性的组态控制. 分析了该结构中电流调控磁涡旋旋性和极性的物理原因和微观机理.     

An Effective Three-Dimensional Micromagnetic Method and Its Application to Magnetic Tunnel Junctions

An effective three-dimensional micromagnetic method for predicting equilibrium configuration of magnetization states is presented with conjugate-gradient technique to minimize the total energy, which has a much faster convergence rate than that of the quasi-Newton method. As an application, magnetic tunnel junctions with pinholes in the ultrathin barrier are simulated. The calculated coupling field Hf increases with the pinhole density increase, corresponding to the decrease of barrier thickness. The free layer domain configuration of tunnel junction during the switching process is also demonstrated.     

O5+离子与He原子碰撞引起的可见光发射

用光学方法测量了O⁵⁺离子(4.06～5.31 kev·amu^-1)与He原子碰撞引起的200～800nm波长范围的可见光发射谱。分析表明,在O⁵⁺与He碰撞中存在着入射离子的单电子俘获激发和双电子俘获激发以及靶原子直接激发过程,并且有较高nl态间的跃迁。经计算得到了各发射谱线的绝对发射截面,并探讨了这些发射截面与入射离子能量之间的依赖关系。     

自旋转移矩效应激发的非线性磁化动力学

本文基于宏观磁矩(macrospin)的Landau-Lifshitz-Gilbert方程,模拟研究了磁性自旋阀结构中由垂直膜面流向的自旋极化电流所激发的磁化转动动力学特性.直流自旋极化电流借助自旋转移矩效应可驱动磁矩翻转或作周期性振荡,交流电可以激发出具有混沌行为的磁矩振荡.展示了磁矩振荡行为随电流强度变化而发生倍周期分岔、直至混沌振荡的行为规律. 关键词： 自旋转移矩效应 微磁模拟 磁性自旋阀 混沌     

Micromagnetic simulation for high field sensors with perpendicular magnetizations

In this paper, we present a micromagnetic design for high field sensors. The hard layer of the sensors is L1垂直磁化;强磁场传感器;微磁学模拟;高巨磁阻效应micromagnetic simulation, giant magnetoresistive, coercivity, demagnetizing fieldProject supported by the Nature Science Foundation of China (Grant No~10404019) and by the Science and Technology Committee of Shanghai (Grant No~05PJ14090).2006-09-232006-11-28In this paper, we present a micromagnetic design for high field sensors. The hard layer of the sensors is L1垂直磁化;强磁场传感器;微磁学模拟;高巨磁阻效应micromagnetic simulation, giant magnetoresistive, coercivity, demagnetizing fieldProject supported by the Nature Science Foundation of China (Grant No~10404019) and by the Science and Technology Committee of Shanghai (Grant No~05PJ14090).2006-09-232006-11-28In this paper, we present a micromagnetic design for high field sensors. The hard layer of the sensors is L10-FePt which is magnetized perpendicularly to film plane and the sense layer is NiFe which is magnetized in the film plane. The magnetization configurations of the hard and sense layers at different external magnetic fields have been simulated. In micromagnetic simulation, the sense field up to one tesla can be reached by using this sensor. We find that whether the sensor has a symmetric or an asymmetric field-sensing window is determined by the coercive field of the hard layer and the demagnetizing field of the sense layer.Corresponding author. E-mail： yaowen@mail.tongji.edu.cn/qk/85823A/200706/24631993.html7000, 7500, 7570P, 7540Mhttp://cpb.iphy.ac.cn/CN/10.1088/1009-1963/16/6/042https://cpb.iphy.ac.cn/CN/article/downloadArticleFile.do?attachType=PDF&id=1092012006-09-23In this paper, we present a micromagnetic design for high field sensors. The hard layer of the sensors is L10-FePt which is magnetized perpendicularly to film plane and the sense layer is NiFe which is magnetized in the film plane. The magnetization configurations of the hard and sense layers at different external magnetic fields have been simulated. In micromagnetic simulation, the sense field up to one tesla can be reached by using this sensor. We find that whether the sensor has a symmetric or an asymmetric field-sensing window is determined by the coercive field of the hard layer and the demagnetizing field of the sense layer.     

GL_C(E)的拓扑结构

设E是实Banach空间,GLC（E）是E上可逆连续线性场全体.本文证明GLC（E）是含有两个道路连通分支的‖·‖L（E）无界拓扑群,并且把这两个连通分支用Leray-Schauder度表示出来.