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magnetic dot
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  “magnetic dot”译为未确定词的双语例句
     Dynamic response of small nanoscale magnetic dot arrays
     纳米磁性颗粒小点阵体系的动力学响应
短句来源
     Novel hysteresis of small nanoscale magnetic dot arrays
     纳米磁性颗粒小点阵体系的奇特磁滞现象
短句来源
     The dynamic response of small single-domain magnetic dot arrays with perpendicular anisotropy is studied numerically via Landau-Lifshitz-Gilbert equations.
     通过数值解Landau Lifshitz Gilbert(LLG)方程,来研究一个具有垂直各向异性的N×N平方点阵结构的单畴铁磁颗粒体系的动力学响应.
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  相似匹配句对
     Dynamic response of small nanoscale magnetic dot arrays
     纳米磁性颗粒小点阵体系的动力学响应
短句来源
     Novel hysteresis of small nanoscale magnetic dot arrays
     纳米磁性颗粒小点阵体系的奇特磁滞现象
短句来源
     Magnetic graphite
     磁性石墨
短句来源
     MAGNETIC HYDROCYCLONES
     磁力水力旋流器
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     DOT Technology and Its Application
     双圆(DOT)隧道技术及应用
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  magnetic dot
In magnetic dot arrays we have explored the genesis of 3D magnetic vortices and determined the critical dot size.
      
In magnetic dot arrays we have explored the genesis of 3D magnetic vortices and determined the critical dot size.
      
We show that the equilibrium vortex phase diagram depends on the size of the magnetic dot and its magnetization, and we discuss the shell structure of the multivortex states with "magic" numbers which are size and magnetization dependent.
      
This commensurate peak effect is enhanced for the magnetic dot arrays when the dots are magnetized in a direction parallel to the applied magnetic field and suppressed when they are anti-aligned.
      
Simulation of Field Coupled Computing Architectures Based on Magnetic Dot Arrays
      
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This summarized paper began to write in 1994 and has been written in every year. In this year it consists of (1) ferrte material with high permeability, (2) new rare earth-transit metal magnetic material, (3) special magnetic property of Mn oxide with perofskite structure, (4) spin-wave mode in submicren magnetic dots and magnetic nanowire, (5) new manufacture technology of Nd-Fe-B system magnetic material.

 这每年撰写的磁性功能材料新进展综述开始于1994年。这次介绍的新进展有:(1)高磁导率铁氧体材料;(2)新的稀土 过渡金属磁性材料;(3)钙钛石型锰氧体的特殊磁性;(4)亚微米磁点和纳米磁线中的自旋波模;(5)Nd Fe B系永磁材料的新制备工艺。

The dynamic response of small single-domain magnetic dot arrays with perpendicular anisotropy is studied numerically via Landau-Lifshitz-Gilbert equations. Three typical magnetic moment configurations are found when the strength of dipolar interaction between particles changes. The configurations are determined by the competition between magnetocrystalline anisotropy and inter-particle interactions. The geometry of the array has an important effect on the reversal of the magnetization vector and...

The dynamic response of small single-domain magnetic dot arrays with perpendicular anisotropy is studied numerically via Landau-Lifshitz-Gilbert equations. Three typical magnetic moment configurations are found when the strength of dipolar interaction between particles changes. The configurations are determined by the competition between magnetocrystalline anisotropy and inter-particle interactions. The geometry of the array has an important effect on the reversal of the magnetization vector and coherent reversal will happen as the dipolar coupling strength increases. When the dipolar interaction between particles is weak, the coherent reversal will be absent, however, the weak dipolar interactions still make a contribution to the moment on which the switching field is applied. When all the moments paralleled to the z axis as the initial state,the minimum switching field for reversing the moment can be much smaller than that for an isolated moment due to the dipolar coupling between moments. But the minimum switching field fast approaches to the value of the minimum switching field for an isolated moment with the increase of the spacing between particles. When all the moments have different initial states,the weak dipolar interaction widens the switching field distribution.

通过数值解Landau Lifshitz Gilbert(LLG)方程,来研究一个具有垂直各向异性的N×N平方点阵结构的单畴铁磁颗粒体系的动力学响应.由于磁性颗粒间的偶极相互作用,我们发现存在三种不同的典型磁矩构形分布.这些构形由磁晶各向异性和磁偶相互作用之间的竞争所决定.磁性粒子的点阵几何构形是影响磁矩翻转的重要因素,偶极相互作用的增强,引起不同位置的颗粒磁矩发生先后顺序的翻转.当初态所有颗粒磁矩都平行于+z方向,且颗粒间的偶极相互作用不足以使磁矩发生耦合翻转,反转某个磁矩所需的最小翻转场将比反转单个(即无偶极相互作用)磁矩时所需的最小翻转场小得多.该种效应随着颗粒间距的增加,将明显地减弱,最小翻转场很快地增加且趋于反转单个磁矩时所需的最小翻转场.当所有颗粒磁矩处于各种不同初态时,弱偶极相互作用加宽了翻转场的取值范围.

 
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