铁磁性坡莫合金纳米环的制备与磁性研究

铁磁性纳米环是一种纳米尺寸的环状实体,由于具备高密度磁存储的能力,被认为是下一代高性能存储器——磁随机存储器(MRAM)的重要结构单元。利用聚苯乙烯微球模板法制备了单分散的坡莫合金Ni75Fe25(NiFe)纳米环,并用扫描电子显微镜(SEM)表征了纳米环的分布情况;用振动样品磁强计(VSM)测量了NiFe纳米环的磁化曲线,显示出两种磁状态,即涡旋态(Vortex state)和双畴态(Onion state),并利用OOMMF软件对NiFe纳米环的磁化翻转过程进行微磁模拟,观察到纳米环不同磁化状态下的自旋组态。     

末端形状对磁纳米薄膜自旋波模式特性的影响

基于微磁学模拟方法研究了磁纳米膜末端形状对自旋波模式特性的影响。获得了多种不同的局域化、量子化自旋波模式特性,以及末端形状对自旋波模式特性的调制规律。通过裁剪纳米膜的末端形状可有效调控边缘模式自旋波特性,存在一临界裁剪参数h0。当裁剪度hh0时,随着h的增大,边缘模式频率快速增加,局域于磁薄膜两末端的磁振荡区域向中央扩展。当h≥h0时,局域于磁薄膜两末端磁振荡在磁体中央合并为一致振荡模式自旋波,边缘模式被抑制。薄膜末端边缘形状对别的自旋波模式特性影响较小。最后,基于近似色散关系理论模型对研究结果进行了解释。     

硅烷偶联剂对磁性纳米微球的磁性能影响

以三氯化铁水溶液作原料,采用部分还原沉淀法,控制一些影响反应的参数。制备了纳米磁微粒子,并用硅烷偶联剂进行了表面修饰。利用透射电镜、红外光谱、X射线衍射等手段对磁微粒子的形貌、结构组成、磁化率、磁响应性进行了表征。结果表明所合成的磁微粒子平均粒径为18nm。分布均匀。具有较强的磁响应性。研究还表明偶联剂的加入会影响磁微粒子的磁性能,其加入量有一个适当值,使得改性后的磁微粒子的磁性能最强。     

纳米磁性高分子微球的合成及磁学性能研究

以PEG/FeOx磁流体为原料,通过乳液聚合方法合成了纳米PS/FeOx磁性高分子微球,并对其进行了表征.微观形貌观察表明产物呈规整球形结构.FT-IR分析表明产物主要由PS、PEG、FeOx组成.XPS分析及元素分析结果表明产物具有核-壳结构.磁学性能研究表明,产物在2～4GHz频段的磁损耗性能较好;产物比饱和磁化强度和磁损耗功率随铁含量的增加而增大.     

镀镍纳米石墨微片的制备及其表征

采用化学镀制备镀镍纳米石墨微片(Ni-nanoG), 对其进行制备工艺研究及结构表征, 旨在得到一种新型导电导磁填料。讨论了硫酸镍浓度、 次亚磷酸钠浓度、 温度、 pH值对石墨微片镀层的影响, 得出镀镍的最佳工艺。采用SEM、 XRD、 EDS对其结构进行了表征, 并用振动样品磁强计(VSM)测试了其磁性能。结果表明: 纳米石墨微片(nanoG)表面镀上了一层紧凑的金属镍。镍均匀分布在nanoG的表面和边界面上, 将nanoG包覆得较严实。 Ni-nanoG厚度约为150 nm。nanoG上镍的含量较高, 其质量分数大约为34.08%。Ni-nanoG的饱和磁化强度为71.2 A·m2·kg-1, 可以作为吸波隐身材料的新型功能型填料。      

基于磁相互作用探索P掺杂对Fe-Si-Nb-Cu-B合金带材组织结构和软磁性能的影响

类金属元素是改善Fe基非晶纳米晶合金非晶形成能力和软磁性能的重要添加剂。用单辊甩带法制备了Fe_73.5Si_13.5Nb₃Cu₁B_9-xP_x(x=0, 3%, 6%, 9%)(原子分数)合金带材,从各元素间磁相互作用出发探索了P替换B对合金组织结构和软磁性能的影响。实验结果表明,P添加可有效提高合金的初晶相晶化温度以及合金的非晶形成能力;但是二次晶化相的析出温度降低,弱化了其热稳定性。当P含量为3%(原子分数)时,合金有较宽的退火温度窗口,且可有效细化初晶相晶粒尺寸,并在525℃退火后表现出最佳软磁性能,此时合金晶粒尺寸为9 nm,矫顽力为0.21 A/m,同时有效磁导率高于x=0合金。但是由于P的添加,残余非晶相中Fe的磁矩降低,导致合金的饱和磁感应强度降低。     

晶化热处理条件对Nd2(FeCo)14B/α-Fe纳米复合材料磁性能的影响

用熔体快淬和晶化处理的方法制备了Nd2(FeCo)14B／α-Fe纳米复合材料。研究了晶化热处理温度和时间对材料磁性能的影响。结果表明Nd2Fe35.5Co2B4.5纳米复合材料的磁性能随热处理条件而变化．较高温度短时间比较低温度长时间热处理样品的磁性能稍好一些，并对其机理进行了研究。     

不同工艺条件对FePt-AlN纳米薄膜磁性影响的研究

利用磁控溅射方法,在加热的单晶MgO(100)基片上制备了以AlN为母体的FePt薄膜,再经过真空热处理后,得到了具有垂直磁各向异性且无磁交换耦合作用的FePt薄膜;同时,研究了掺杂AlN含量、薄膜的厚度及退火温度对薄膜的磁性能的影响.结果表明,非磁性相AlN的添加能够降低磁交换耦合作用,但同时也会破坏薄膜的垂直磁各向异性.降低薄膜厚度,有利于改善薄膜的垂直磁各向异性,FePt-AlN薄膜的厚度为6nm且掺杂AlN含量达到40%时,经650℃热处理1h后薄膜具有良好垂直磁各向异性、适中矫顽力且无磁交换耦合作用.     

磁场热处理对Ｎd2Fe14B／α—Ｆe纳米材料磁性和微磁结构的影响

对Ｎd2Fe14B/a－Ｆ基纳米交换耦合磁体进行了磁场热处理的研究,研究发现,退火温度在硬磁相居里点附近时（３００~400℃）有明显的处理效果,磁场处理可加强磁性相之间的耦合,提高磁体的顽力和剩磁比,磁场可以引发晶粒间的相对滑动和调整,低熔点金属Ｉn的少量添加有助于在外磁场中晶粒的转动。     

片层纳米结构磷酸铁制备及对磷酸铁锂电性能的影响

采用液相反应结晶法,在磷源及铁源中添加NaAlO_2,利用在结晶过程中生成的Al(OH)3胶体对结晶面的作用,合成出具有片层纳米结构纺锤体状磷酸铁前驱体,并通过高温固相法进一步制备成磷酸铁锂。采用XRD、FT-IR、SEM、TEM、比表面及孔隙率分析、激光粒度分析和电化学性能测试等手段对样品进行表征分析。结果表明,由具有片层纳米结构的磷酸铁前驱体制备的磷酸铁锂比由无片层纳米结构的磷酸铁前驱体制备的磷酸铁锂在0.1C下的首次放电容量提升了20%,达到151.48mAh/g,电极电荷转移电阻降低了约75%,仅为27.23Ω;0.1C倍率下循环50次后容量保持率可达96%。同时,对Al(OH)3胶体影响片层纳米结构磷酸铁生成机制进行了分析和讨论。     

直径对玻璃包覆非晶合金微丝磁性的影响

采用Taylor-Ulitovsky方法制备了直径分别在6.3～28.0μm、20.2～28.0μm和14.0～35.2μm之间的玻璃包覆非晶态FeCuNbVSiB、FeBSiCMn和CoNiFeSiB微丝。通过X射线衍射、扫描电镜、振动样品磁强计分别测试了玻璃包覆微丝的组织结构、微观形貌和磁性,研究了不同成分玻璃包覆磁性合金微丝的玻璃包覆层厚度、合金芯直径对微丝磁性能的影响。结果表明了,玻璃包覆磁性合金微丝的磁性能的影响因素由大到小依次为：饱和磁致伸缩系数、微丝成分和微丝尺寸。轴向磁化时随着微丝直径及玻璃包覆层厚度的增大,3 种微丝的径向饱和场强度降低,FeCuNbVSiB和FeBSiCMn微丝的轴向矫顽力先分别由508 A/m和390 A/m降低到486 A/m和278 A/m后再升高到2570 A/m和342 A/m,CoNiFeSiB微丝的轴向矫顽力由171 A/m降低到63 A/m。     

玻璃包覆磁性微丝的制备及微波电磁性能

采用Taylor-Ulitovsky方法制备了Fe基和Co基非晶态玻璃包覆微丝,测试并分析了玻璃包覆微丝的微结构、微观形貌、静磁性能及其微波复磁导率和复介电常数.研究结果表明,通过改变拉丝速度,可以制备出直径6.3～23.5μm的非晶态玻璃包覆微丝;制备时通过水冷或气氛保护可以控制样品的物相组成.典型样品的各项异性等效场高达7.96×103A/m.Fe基样品磁导率在6.3GHz具有自然共振峰,Co基样品在所测频率范围没有共振峰,此测量结果和根据理论计算的自然铁磁共振频率基本一致.典型样品的相对微波复介电常数均低于25且随频率升高而降低.     

反铁磁层厚度对垂直磁各向异性钴/铂/铁锰多层膜磁性质的影响

在室温下用超高真空磁控溅射系统制备了一系列的Pt(4.0nm)/[Co(0.5nm)/Pt(0.3nm)]3-FeMn(tAFnm)多层膜样品,研究了反铁磁层厚度对于易轴垂直于样品表面的Co/Pt/FeMn多层膜磁性质的影响。在室温下利用样品的剩磁进行了X射线磁圆二色测量(XMCD),结果表明在铁磁/反铁磁界面有反铁磁层铁锰的净磁矩,这些净磁矩仅来自于铁元素。铁的磁矩倾向于垂直于膜面排列。磁测量结果表明,随着铁锰层厚度的增加,交换偏置场HEB增加直到饱和,而HC先增加,然后轻微减少,在tAF7.5nm以后,HEB和HC都几乎不变了。没有观察到磁锻炼效应。     

Effects of magnetic fields on cracks in a soft ferromagnetic material

The 2D problem of a soft ferromagnetic solid with a finite crack under a uniform magnetic field has been studied based on the linear theory of Pao and Yeh. Especially, in this work, the Maxwell stresses induced by the applied magnetic field are taken into account in the boundary conditions not only along the crack surfaces, but also at infinity. Based on these boundary conditions, the related boundary-value problem is solved by using Muskhelishvili’s complex variable method to obtain the complex potentials. Thus, it is found that the obtained complex potentials are constant, which indicates that both magnetic fields and stress are uniform in the solid. This implies that if only a pure magnetic field is applied, it has no effects on a crack in a soft ferromagnetic solid. To confirm this result, the same boundary-value problem is solved by the integral transform technique, which shows the same finding as that by using the complex variable method. This outcome is consistent with available experimental data but different to previously published theoretical results.     

Soft magnetic properties of hybrid ferromagnetic films with CoFe, NiFe, and NiFeCuMo layers

Two-layered ferromagnetic alloy films (NiFe and CoFe) with intermediate NiFeCuMo soft magnetic layers of different thicknesses were investigated to understand the relationship between coercivity and magnetization process by taking into account the strength of hard-axis saturation field. The thickness dependence of H_EC (easy-axis coercivity), H_HS (hard-axis saturation field), and χ (susceptibility) of the NiFeCuMo thin films in glass/Ta(5 nm)/[CoFe or NiFe(5 nm-t/2)]/NiFeCuMo(t = 0, 4, 6, 8, 10 nm)/[CoFe or NiFe(5 nm-t/2)]/Ta(5 nm) films prepared using the ion beam deposition method was determined. The magnetic properties (H_EC, H_HS, and χ) of the ferromagnetic CoFe, NiFe three-layers with an intermediate NiFeCuMo super-soft magnetic layer were strongly dependent on the thickness of the NiFeCuMo layer.     

脉冲磁场激励下铁磁梁式板动力响应特征研究

基于广义变分原理得到磁力计算模型和磁场摄动技术,研究了不可移简支铁磁梁式板在矩形和锯齿形两类典型脉冲磁场作用下的磁弹性动力响应特征及动力失稳现象。数值模拟了铁磁梁式板在稳恒磁场,脉冲磁场下的振幅,频率的变化及其动力失稳特征。揭示了脉冲磁场的形状,脉冲持续时间,脉冲幅值与铁磁梁式板振幅,频率,临界失稳磁场值等特征参量之间的关系,为工程实际中铁磁结构的安全设计和可靠性评估提供依据和参考。     

Influence of magnetic annealing on high-frequency magnetic properties of FeCoNd films

FeCoNd thin film with thickness of 166 nm has been fabricated on silicon (1 1 1) substrates by magnetron co-sputtering and annealed for one hour under magnetic field at different temperatures (T_a) from 200 °C to 700 °C. The As-deposited and annealed FeCoNd film samples at T_a ≤ 500 °C were amorphous while the ones obtained at T_a ≥ 600 °C were crystallized. We found that the perpendicular anisotropy field gradually decreases as the annealing temperature increases from room temperature to 300 °C. A well induced in-plane uniaxial anisotropy is achieved at the annealing temperature between 400 and 600 °C. The variation of the dynamic magnetic properties of annealed FeCoNd films can be well explained by the Landau-Lifshitz equation with the variation of the anisotropy field re-distribution and the damping constant upon magnetic annealing. The magnetic annealing might be a powerful post treatment method for high frequency application of magnetic thin films.     

Effect of Mn substitution on structural and magnetic properties of ferromagnetic shape memory alloys

The structure and the magnetic transitions have been investigated as a function of Mn in stoichiometric Ni₂MnGa heusler alloys. Particular attention is paid to examine the linear increase of martensite transformation temperature on substituting Mn for Ga. It is observed that the martensite temperature increases and Curie temperature decreases with the effect of Mn content. Room-temperature magnetic measurements show the composition-dependent characteristics with decreasing magnetic saturation values and increasing coercivity values due to decrease in the magnetic exchange interaction strength with increasing Mn in place of Ga. The scanning electron microscopy image confirms that the Mn-rich alloys have the martensitic plates.     

Experimental insight into the magnetic and electrical properties of amorphous Ge1-xMnx

Abstract

We present a study of the electrical and magnetic properties of the amorphous Ge_1-xMn_x.DMS, with 2% ≤ x ≤ 17%, by means of SQUID magnetometry and low temperature DC measurements. The thin films were grown by physical vapour deposition at 50°C in ultrahigh vacuum. The DC electrical characterizations show that variable range hopping is the main mechanism of charge transport below room temperature. Magnetic characterization reveals that a unique and smooth magnetic transition is present in our samples, which can be attributed to ferromagnetic percolation of bound magnetic polarons.