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单轴各向异性的英文

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"单轴各向异性"怎么读用"单轴各向异性"造句

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  • uniaxial anisotropy

例句与用法

  • Analysis of near - field distribution and cross - polarization radiation pattern cavity - backed microstrip patch antenna on a uniaxial substrate
    单轴各向异性背腔式微带贴片天线的表面缝隙场分布及交叉极化方向图分析
  • At first , the 3 - d theoretical model of photothermal radiation was built in the cylindrical coordinate axes , by reviewing thermally uniaxial materials irradiated by continuously modulated beam
    先是考察将热单轴各向异性材料在连续调制光辐照下,在柱坐标系下建立光热辐射测量( ptr )技术的三维理论模型。
  • The perpendicular anisotropy and in - plane uniaxial anisotropy decrease with increasing film thickness . the oscillatory curve of hres is asymmetrical , which requires an additional term of anisotropy with four - fold symmetry to fit
    4ml后,薄膜形成连续膜,垂直利平面的单轴各向异性随膜厚的增加而减小,并出现了四度对称的成份。
  • ( 2 ) the oscillatory curve of hres is asymmetrical for films . it originates mainly from the lower resonance field hres comparing with anisotropy field , which causes deviation of the direction of magnetic field from that of magnetization
    与fe gaas系统的平面单轴各向异性相比, fe inas系统的平面单轴各向异性消失得较快,这可能是fe inas系统各向异性的应力弛豫比fe gaas系统快所致。
  • The major findings are listed below : ( 1 ) the film of 4 . 1 ml consists of superparamagnetic nano - cluster with large perpendicular anisotropy and in - plane uniaxial anisotropy . the oscillatory curve of is symmetrical which can be described by a function of sin square
    Iml时,未形成连续薄膜,而是超顺磁性的团簇,具有很大的单轴的垂直各向异性和平面单轴各向异性,色散关系曲线是对称的正弦类曲线。
  • The anisotropy of four - fold symmetry indicates the appearance of cubic anisotropy . ( 4 ) the in - plane unixial anisotropy existed in films originates probably from magneto - elastic interaction due to the anisotropic strain caused by lattice mismatch at the interface
    ( 3 )薄膜中存在的面内单轴各向异性可能来源于磁弹性相互作用,这是由于薄膜在生长过程中,与衬底的品格错配而产生的应力各向异性导致的。
  • 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。
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