共查询到17条相似文献,搜索用时 125 毫秒
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采用交换相互作用的分子场理论模型对金属间化合物HoMn6Sn6的自旋重取向相变进行了研究. 从理论上计算了HoMn6Sn6的易磁化方向以及Ho和Mn离子磁矩与c轴夹角随温度的变化. 基于单离子模型计算了Ho离子的一阶和二阶磁晶各向异性常数K1R和K2R随温度的变化. 研究表明,为了很好描述该化合物的自旋重取向相变,必须考虑Ho离子的四阶晶场项及相应的二阶磁晶各向异性常数K2R,K2R与K1R和Mn离子磁晶各向异性常数K1t之间的相互竞争是导致HoMn6Sn6自旋重取向相变的重要因素.
关键词:
稀土-过渡族金属间化合物
自旋重取向
磁晶各向异性 相似文献
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针对低温下各向同性Pr2Fe14B永磁材料的最小形核场问题,用数值 计算法和近似解 析解研究了第二磁晶各向异性常数K2对最小形核场的影响.研究发现,尽管对于 Nd2 Fe14B永磁材料一级近似的解析解与数值计算结果很接近,但是对于低温下各向 同性P r2Fe14B永磁材料则至少要用二级近似下的解析解才能与数值计算 结果相接近.用有 关最小形核场的计算结果很好地解释了低温时各向同性Pr2Fe14B永 磁材料的矫顽力与最小形核场的关系.
关键词:
第二磁晶各向异性常数
形核场
矫顽力 相似文献
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LaBaMnO薄膜的铁磁共振 总被引:1,自引:1,他引:0
用电子自旋共振实验研究La0.65Ba0.35MnO3(LBMO)薄膜的磁性,从磁性膜的各向异性铁磁共振谱得到不同角度θh时的共振磁场Br,求出样品的等效磁场Beff及旅磁比γ,并通过样品的饱和磁化强度Ms,求出各向异性常数K. 相似文献
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本文通过同时测量金属玻璃Co65.2Fe4.2Ni3Nb1Al2Si9.8B14.8的同一样品在各种横磁张力退火后的磁各向异性、磁致伸缩和应变,对这些物理量的变化情况作了比较。应变感生各向异性和暂态蠕变的行为有某种相似性,但其间不存在对应或因果关系。磁化感生各向异性Kum,应变感生各向异性Kus,饱和磁致伸缩常
关键词: 相似文献
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对纳米晶Fe73.5Cu1Mo3Si13.5B9合金的原始制备态和各退火态样品进行了室温Mossbauer谱研究,结果表明晶化态的合金存在α-Fe(Si)微晶相和晶界的非晶相。晶相和非晶相内场和面积随退火温度的变化是退火时Cu,Mo,B等成分的扩散和在各相中的再分配引起的。最佳磁性能对应非晶相中的铁量占合金铁总量的30%左右,超微晶合金的双相无规各向异性模型表明,一定量的非晶相对保持纳米晶优异的软
关键词: 相似文献
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对多晶Y3Fe3Fe5-xMnxO12(x=0.05和0.09),得到300K下的中子衍射曲线。发现当x=0.05时,Mn3+离子占据16a和24d位置的几率分别为0.72和0.28;当x=0.09时,Mn3+离子全部占据16a位置;还得到两种组分16a和24d位置各自的磁矩值。在外磁场(800—10KOe)下测量Y3Fe5-xMnxO12(x=0—0.11)的磁化曲线,温度范围是1.5—300K。得到饱和磁矩值;并利用趋近饱和定律确定1.5K下的磁晶各向异性常数k1值,发现|k1|值随含锰量增加而减小。
关键词: 相似文献
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用原子力显微镜(AFM)观测了不同张应力退火的Fe基纳米晶(Fe73.5Cu1Nb3Si13.5B9)薄带横断面的形貌,并结合X射线衍射(XRD)图谱对不同张应力退火的Fe基纳米晶薄带的介观结构进行分析;测量了不同张应力退火Fe基纳米晶薄带的纵向驱动巨磁阻抗(LDGMI)曲线及横向磁各向异性场;认为张应力退火Fe基纳米晶薄带感生横向磁各向异性场的介观结构机理,是由于外加张应力退火产生由非晶相包裹着的α-Fe(Si)纳米晶粒(包裹晶粒)的横向优势团聚.
关键词:
应力退火
介观结构
AFM
团聚 相似文献
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E. N. Sheftel’ S. V. Komogortsev R. S. Iskhakov P. K. Sidorenko L. A. Chekanova N. S. Perov A. N. Ivanov 《Bulletin of the Russian Academy of Sciences: Physics》2010,74(10):1449-1451
The magnetic properties (magnetization curve, ferromagnetic resonance spectrum) of nanocrystalline Fe79Zr10N11 films obtained by RF magnetron sputtering with subsequent annealing were studied experimentally, along with the fundamental
magnetic constants of these films (saturation magnetization M
S, local magnetic anisotropy energy K, and the exchange coupling constant A). The magnetic properties are discussed within the random magnetic model, which determines the correlation of the magnetic
properties with the fundamental magnetic constants and nanostructure parameters (grain size, magnetic anisotropy, and correlation
radius R
C). The exchange correlation length 2R
L
for the film magnetic microstructure was determined by correlation magnetometry. 相似文献
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Kopcewicz M. Grabias A. Idzikowski B. Williamson D. L. 《Hyperfine Interactions》2002,139(1-4):525-534
The specialized rf-Mössbauer technique is used to elucidate the magnetic properties of NANOPERM-type nanocrystalline alloys. The influence of alloy composition on the soft magnetic properties is studied for the Fe80M7B12Cu1 (M: Ti, Ta, Nb, Mo, Zr) alloys. The rf-Mössbauer experiments allowed us to distinguish magnetically soft nanoclusters from magnetically harder microcrystalline phases. The measurements performed as a function of the rf field intensity allowed the determination of the distribution of anisotropy fields related to the size distribution of bcc nanoclusters. Smaller anisotropy fields in the nanocrystalline phase were found in Nb-, Zr-, and Mo-containing alloys as compared with the alloys which contain Ti and Ta. The Mössbauer measurements were supplemented by X-ray diffraction determination of the size of nanocrystalline grains. 相似文献
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An experimental determination (both direct and indirect) of the characteristics of the magnetic microstructure, namely, the ferromagnetic correlation radius R f and the rms fluctuation of the mean anisotropy D 1/2〈H a〉, is performed for amorphous and nanocrystalline ferromagnets with a random anisotropy characterized by the quantities R c and D 1/2 H a, respectively. The magnetization curves of amorphous and nanocrystalline ferromagnets are found to exhibit a dependence on H that is caused by the alignment of the magnetizations of individual magnetic blocks with the field. 相似文献