crystalline anisotropy meaning in Chinese
晶态蛤异性
晶态各向异性
晶体蛤异性
晶体各向异性
Examples
- Influence of site preference of al atoms on magneto crystalline anisotropy of gd2co17 compounds
17化合物磁晶各向异性的影响 - Simulation of magneto - crystalline anisotropy energy of cold rolled non - oriented silicon steel
冷轧无取向硅钢的磁晶各向异性能的模拟 - Moke and fmr studies were performed on epitaxial single crystalline fe ph . d thesis ; investigations of magnetic properties on magnetic thin , ultrathin and patterned films ultathin films on iii - v semiconductor inas substrate with thickness of 8 - 25monolayer ( ml ) . the major findings are listed below : ( 1 ) the in - plane magnetic crystalline anisotropy of film with 8 - 25 ml thick are four - fold anisotropy , and the in - plane unixial anisotropy of fe / inas films decreses faster with thickness than that in fe / gaas films . it could be explained that the stain relaxation of fe / inas films is also faster than that in fe / gaas films as indicated by leed
对于外延生长在inas衬底上、厚度为8 - 25ml的超薄fe单晶膜进行了铁磁共振和磁光研究，获得以下几点结果： ( 1 )膜厚在8 - 25ml之间时，薄膜面内的磁晶各向异性为四度对称各向异性，垂直单轴各向异性比同厚度的fe gaas系统小许多，而立方各向异性则比fe gaas系统更接近bcc结构的fe 。 - Moke and fmr studies were performed on single crystalline fe ultathin films epitaxially grown on iii - v semiconductor gaas substrate with thickness 4 . 1 - 33 monolayer ( ml ) . a theoretical mode for fitting fmr experimental data was established . the results demonstrated the structures and reproduced the evolution of the magnetic properties of ultrathin films with various thickness from the state of superparamagnetic nano - cluster through coexistence of two magnetic phases to continuous film , especially the change of magnetic crystalline anisotropy from unixial to cubic
1 - 33原子层厚度( monolayer ,简称ml )的fe单晶超薄膜进行了铁磁共振( fmr )和磁光研究，建立了理论模型对铁磁共振实验结果进行了模拟，重现了不同厚度的超薄膜，从纳米团簇到两相共存的过度阶段直至连续薄膜结构与磁性的变化，特别是磁各向异性从单轴各向异性向立方各向异性转变的演化过程。