GdFeCo磁光薄膜飞秒激光感应反常磁滞回线研究*

该文使用飞秒时间分辨泵浦-探测磁光克尔光谱技术,研究了飞秒激光加热GdFeCo磁光薄膜跨越铁磁补偿温度时,净磁矩方向发生转变而引起磁化反转的反常克尔磁滞回线。通过测量不同激发功率下以及不同泵浦脉冲数下的反常克尔回线,揭示反常回线包含连续脉冲激发产生的积累效应以及外场磁化史的记忆效应,对反常回线的形成起源做了深入探索和详细研究。研究结果对于深入理解GdFeCo合金薄膜中稀土-过渡金属间的反铁磁耦合特性以及磁化反转的机理具有重要意义。     

Ni-Fe氧化物复合磁性纳米微粒及其磁性液体的磁化性质

 用共沉淀法制备了Ni-Fe氧化物复合磁性纳米微粒,并采用Massart法合成了无表面活性剂的离子型磁性液体。用X射线衍射仪（XRD）、X射线能谱仪（EDX）、X射线光电子能谱仪（XPS）、透射电子显微镜（TEM）分别对其微粒结构及粒径进行分析,并用HH-15振动样品磁强计（VSM）测量了磁性微粒和磁性液体的磁化强度,分别用Langevin理论和类气压缩模型对磁性液体磁化曲线进行拟合。实验结果表明,Langevin理论曲线与实验曲线有较大偏差,而类气压缩模拟的曲线与实验曲线拟合的较好,且压缩参数γ随磁性液体体积分数的增大而增大。应用场致团聚效应解释了Ni₂O₃/γ-Fe₂O₃磁性液体的磁化性质。     

BiFeO_3多铁Landau模型的修正

考虑到Landau自由能在平衡态时必须是稳定的以及Landau唯象模型中的每一个序参量都必须是实数,BiFeO_3材料的Landau自由能展开系数被重新计算.利用这些参数,模拟了电滞回线、磁滞回线和随外加磁场变化的磁电耦合系数,理论结果与最近报道的实验结果吻合得很好.     

纳米Fe_3O_4颗粒的制备及磁性能

采用X-ray衍射、高能X-ray衍射、透射电子显微镜及振动样品磁量计等表征手段,研究了不同制备工艺对Fe3O4纳米粒子的平均晶粒尺寸及磁性能的影响.结果表明多元醇方法所制备的Fe3O4粉体平均粒径为32 nm,其饱和磁化强度为6.8×10-3A/m(该值比块体Fe3O4的饱和磁化强度约降低了8%),剩磁Mr=4.2×10-3A/m,矫顽力Hc=1.43×10-2T;通过共沉淀方法得到的Fe3O4粉体平均粒径显著减小为7 nm,但是其饱和磁化强度也明显降低为3.3×10-4A/m,比块体Fe3O4的饱和磁化强度减小约96%,剩磁及矫顽力也下降为零.这是由于小尺寸效应导致出现超顺磁现象,说明Fe...     

Tb（3-x）YxFe26.5Cr2.5（0.3≤x≤2.5）化合物的结构和低温磁性

采用X射线衍射和磁性测量等方法,研究了Tb3-xYxFe26.5Cr2.5化合物的结构和低温磁性.当0.3≤x≤2.5时,化合物呈现Nd3(Fe,Ti)29型单斜结构,属于A2/m空间群.化合物晶胞体积V和居里温度TC随Y含量增加而减少.随着Y含量的增加,低温自发磁化强度M0、饱和磁化强度Ms和各向异性场Ba均降低,出现一级磁化过程.     

甘氨酸燃烧法制备纳米晶CoFe2O4铁氧体及烧结温度对其磁性能的影响

利用甘氨酸作为燃料和配合剂, 采用自蔓延燃烧法制备纳米晶钴铁氧体, 并通过X射线衍射、 扫描电子显微镜和振动样品磁强计表征样品的结构和磁性能. 结果表明, 平均晶粒尺寸对样品的磁性能影响较大, 晶粒尺寸随烧结温度的变化而变化, 并得到了矫顽力H_c和比饱和磁化强度σ_s随烧结温度的变化曲线.      

Effect of vacuum annealing on the characteristics of composite pellets containing DBSA-doped polyaniline and Fe nanoparticles

The DBSA-PANI-Fe composite powder with 50wt% of Fe nanoparticles was prepared by mechanically mixing the DBSA-doped polyaniline powder and Fe nanoparticles. The composite powder was compacted to pellets and the pellets were annealed in vacuum at 443,493,543, and 593 K for 60 and 120 min. The conductivity of the pellet increases markedly with increasing the annealing temperature up to 493 K, and then decreases with further increasing the annealing temperature. When the pellet was annealed at 493 K for 60 min, the increment of conductivity reaches a maximum value, and the conductivity is 2.6 times as large as that of the pellet unannealed. The conductivities of the pellets annealed under the conditions of 543 K/120 min, 593 K/60 min, and 593 K/120 min are lower than the conductivity of the pellet unannealed. For all the pellets, the variation in conductivity with temperature reveals that the charge transport mechanism can be considered to be 1-D variable-range-hopping (1-D VRH). The composite pellet shows a magnetic hysteresis loop independent of the annealing condition. The saturation magnetization is about 5.4×104 emu/kg. The saturation field and the coercivity are estimated to be 4.38×105 and 3.06×104 A/m, respectively. The crystalline structure ofFe nanoparticles in the composites does not change with the annealing condition. The annealing condition cannot destroy the polymer backbones.     

Epitaxial growth of Fe/Ag single crystal superlattices and their magnetic properties

Single crystal Fe/Ag(001) superlattices with various periodicities were fabricated using ultrahigh vacuum evaporation deposition. It was found that single crystal bcc Fe layers and single crystal fcc Ag layers can epitaxially grow on a single crystal Ag buffer layer alternately, which was deposited on NaCl single crystal chips by ion beam assisted deposition. The magnetic measurements of the superlattices reveal an oscillation coupling between ferromagnetism and antiferromagnetism as a function of the Ag layer thickness. The oscillation period, which is 1 nm (5 Ag layers), is in good agreement with the calculated values when the Ag thickness is greater than 1.5 nm. While the thickness of the Ag spacer layer decreases to 1 nm, the oscillation coupling varies from calculations, which can be attributed to the intermixing of the interlayers according to the annealing results.     

低居里点FeCrB非晶合金的磁热效应

基于输电线路抗覆冰的应用背景,通过对Fe100-x-yCrsBy（x=11～20,y=9-20）的成分调节和快淬工艺参数控制,制备了同时具有低居里温度和高饱和磁极化强度的非晶带材．测试研究表明Fe65Cr15B20和Fe64Cr16B20的居里温度分别为28．6和11．6℃,Fe65Cr15B20和Fe64cr16B20在0℃的饱和磁极化强度分别为0．69和0．62T．设计组装了一种近似绝热磁致热功率的测量装置,用该装置对Fe65cr15B20和Fe64cr16B20两种非晶合金带的磁热功率进行了近似测量和分析．     

Magnetic properties of perpendicularly orientated L1<Subscript>0</Subscript> FePt nanoparticles

L10 FePt films were deposited on MgO (001) substrates heated to 700°C by magnetron sputtering.Assisted by the misfit of lattice between film and substrate,strong (001) texture was formed.The film at nominal thickness t N=5 nm was composed of nanoparticles with a size of～70 nm,and showed a high coercivity of～105 kOe at 4.2 K.At t N=～50 nm,as the film changed from discontinuous to continuous,the coercivity dropped about one order of magnitude.Micromagnetic simulation implies that the magnetization reversal is...