1) anisotropic magnetostatic field
各向异性磁场
2) anisotropyfield
磁各向异性场
3) magnetic crystal anisotropy field
磁晶各向异性场
1.
The saturation magnetization M s and Curie temperature T c decreases with increasing x ,but the magnetic crystal anisotropy field H a increases with increasing x .
随着x的增加 ,饱和磁化强度减小 ,居里温度下降 ,磁晶各向异性场增加。
4) magnetocrystalline anisotropy field
磁晶各向异性场
1.
Their magnetocrystalline anisotropy field can be varied from 200kA/m to 1140kA/m.
结果，取向度大于７５％，介电损耗小于５×１０－３，饱和磁化强度为３６６ｋＡ／ｍ几乎不变，磁晶各向异性场为２００ｋＡ／ｍ≤Ｈａ≤１１４０ｋＡ／ｍ，这类材料可应用于Ｘ至Ｋａ波段的微波器件。
2.
A calculation of temperature dependence of magnetocrystalline anisotropy fields in Sm2Fe17Cx (x = 0.
用单离子模型计算了不同温度下Sm2Fe17Cx化合物磁晶各向异性场，结果与实验基本吻合。
5) magnetic anisotropy
磁各向异性
1.
Element-specific in-plane magnetic anisotropy in Co_(0.9)Fe_(0.1) films;
Co_(0.9)Fe_(0.1)薄膜面内元素分辨的磁各向异性
2.
Thermal annealing at 100℃ shows that large perpendicular magnetic anisotropy and coercivity still remain after annealing,inverse magnetostrictive anisotropy and coercivity still remain after annealing,inverse magnetostrictive anisotropy is one part of perpendicular magnetic anisotropy and responsible for the decrease of coercivity.
10 0℃退火表明 ,薄膜保留较大的垂直磁各向异性、矫顽力和很好的矩形比 ,磁致伸缩各向异性是引起矫顽力下降的主要原因。
3.
The magnetic anisotropy constants of the samples with various grain size were obtained by the studies of collecti.
通过对集体磁激发现象的研究，得到了不同颗粒尺寸的α－Ｆｅ_２Ｏ_３超微粒的磁各向异性能常数。
6) anisotropy field
各向异性场
1.
It was discussed by anisotropy field that the parallel magnetization to the c-axis is negative when/ar= 0.
当外磁场等于零或者较小时,难磁化方向的磁化强度为负值,利用各向异性场对此进行了解释,并由ESR谱计算出了各向异性场。
2.
The magnetocrystalline anisotropy field at room t.
２之间呈现极大值，各向异性场Ｂａ随ｘ的增加，先增加而后减小
补充资料：各向异性第三临界磁场（anisotropicthirdcriticalmagneticfield）
各向异性第三临界磁场（anisotropicthirdcriticalmagneticfield）
在主轴坐标系中，设磁场平行于主轴Z，对有表面超导电性存在的各向异性超导样品，由各向异性GL方程给出的各向异性第三临界磁场为
Hc3∥(T)=(1.69)Hc2∥(T)
这里Hc2∥(T)为磁场平行主轴Z时样品的第二临界磁场（见“各向异性第二临界磁场”）。若有效质量m1*=m2*，则过渡到x-y面是各向同性的情形。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条