水热法掺杂的Yb^3＋对NiYbxFe2-xO4铁氧体磁性和形貌的影响

本文以研究稀土元素镱掺杂对镍铁氧体磁性能的影响用为目的,采用水热法,去离子水作为溶剂,用硝酸镍（Ni（NO3）2·6H2O）,硝酸铁（Fe（NO）3·9H2O）,硝酸镱Yb（NO3）3·5H2O,氢氧化钠（NaOH）为原料,制备出镍铁氧体NiYbxFe2-xO4纳米粉体.利用X射线衍射（XRD）,X射线能谱仪（EDS）,扫描电镜（SEM）,透射电子显微镜（TEM）,振动样品磁强计（VSM）在成分,定性定量和形貌等方面进行了表征.结果表明,稀土元素镱掺杂将会降低镍铁氧体纳米粉体的晶粒尺寸.稀土离子磁矩的磁稀释作用导致镍铁氧体纳米磁性材料的饱和磁化强度降低,并且随着掺杂量的逐渐增加,样品的饱和磁化强度和矫顽力逐渐降低.     

粉末压片法XRF分析锰锌铁氧体磁性材料的成分

试样经研磨、过筛,硼酸垫底,压成片样,用X射线荧光光谱法（XRF）测定锰锌铁氧体Mn3O4、ZnO、Fe2O3成分含量,同时自制一套参考标样作标样。方法快速、精确、稳定,可以满足生产及研发定量分析要求。     

纳米Zn0.6CoxFe2.4－xO4晶粒的结构相变与磁性研究

采用溶胶 凝胶自燃烧法制备了纳米尺度的锌钴铁氧体Zn06CoxFe24-  xO4(x=0—030)粉体,分别在不同温度下进行了热处理，利用x射线衍射仪(XRD) 和振动样品磁强计(VSM)对其物 相结构和磁性进行了测量和分析.实验结果表明，锌钴铁氧体Zn06Co015Fe 225O4在550—800℃温度区间出现α Fe2O3过渡相，在高于800℃温度时生 成 单一尖晶石相锌钴铁氧体；随钴含量的增加，Zn06CoxFe2 关键词： 锌钴铁氧体 磁性 结构 相变 溶胶 凝胶     

离子型钴铁氧体磁流体的稀土改性与机理研究

采用化学共沉淀法以柠檬酸三钠为表面改性剂制备了离子型稀土复合钴铁氧体磁流体.利用X衍射仪和透射电镜对磁粒子的组成、结构及粒径进行了分析.利用古埃磁天平和分光光度计研究了稀土离子改性对磁流体饱和磁化强度和磁感应的影响,实验结果表明:合成过程中添加稀土离子能明显降低磁性纳米粒子的粒径,制得的磁粒子均呈球形,钴铁氧体磁粒子的粒径为12～15nm,稀土钴铁氧体磁粒子的粒径为6～8nm.利用稀土改性的微观模型解释了粒径的降低.添加Dy3+能提高饱和磁化强度和磁感应,添加Y3+则能提高磁感应,却降低了饱和磁化强度.并从理论上对其改性机理进行了详细的分析.     

纳米晶复合SrFe12O19γ-Fe2O3永磁铁氧体的制备和交换耦合作用

采用solgel方法制备M型六角锶铁氧体.利用X射线衍射,透射电子显微镜和VSM对纳米晶样品进行了研究.当焙烧温度小于或等于800℃,样品存在复相.在同样条件下,压成薄片的样品呈现了硬磁与软磁SrFe12O19γFe2O3的纳米复合相的磁性交换耦合作用.800℃焙烧的薄片样品的比饱和磁化强度σS为75.6A·m2kg,内禀矫顽力HcJ为478.9kAm,最大磁能积(BH)max为14.9kJm3,而粉末样品相应的分别为75.9A·m2kg,509.6kAm和12.1kJm3.当焙烧温度大于850℃时,只有 关键词： 六角锶铁氧体 纳米复合 交换耦合 磁性     

聚苯胺/钡铁氧体复合材料的制备及电磁性能

"采用原位掺杂聚合法,将聚苯胺对粒径在60~80 nm的M型钡铁氧体颗粒(BaFe12O19)进行包覆,得到了具有导电性和磁性的复合材料．通过X射线衍射、傅利叶变换红外光谱仪、扫描电镜和透射电镜等测试手段对材料的形貌和结构进行了表征．结果表明：PANI链段与BaFe12O19颗粒之间存在着作用力．使用振动磁强计和四探针法测定了复合材料的磁性能与电性能,其中50%复合材料的饱和磁化强度为22.2 emu/g,电导率为0.069 S/cm．"     

微颗粒X射线荧光强度MCNPX模拟与WDXRF实验

为研究样品微颗粒在X射线荧光(XRF)分析中对测量结果的影响,运用蒙特卡罗模型MCNPX对X射线荧光仪进行建模,研究了样品颗粒粒径对X射线荧光特征峰强度、峰总比和源峰探测效率的影响,并设计波长色散X射线荧光光谱法(WDXRF)分析实验对模拟结果进行了检验。结果表明：对于样品微颗粒X射线荧光强度与粒径尺寸的关系,MCNPX模拟值与理论计算值保持一致;MCNPX模拟结果与WDXRF实验结果存在一定差异,这取决于MCNPX模型对待测样品状态的假设与实际情况存在一定的差异性;运用样品粉碎、研磨至小颗粒并进行压片处理的办法,可使WDXRF实测结果尽可能的减小与MCNPX理论模拟结果的差异性;在待测样品的颗粒粒径达到一定尺寸时,其峰总比、源峰探测效率、特征峰X射线荧光计数均趋于稳定值;颗粒粒径在某一特定尺寸范围之内,颗粒度效应的影响不容忽视;除此之外,颗粒度效应的影响基本可以忽略。论文充分考虑了待测样品颗粒粒径对XRF分析结果的影响,为减小因颗粒度效应引起分析结果的不确定性提供了一种可行的研究思路,该方法也可为X射线分析的生产实践提供一定的技术参考。     

燃烧法制备纳米CdFe2O4及表征

以Fe（NO3）3.9H2O和Cd（NO3）2.4H2O为原料,以柠檬酸为还原剂,采用燃烧法制备了CdFe2O4纳米粉体,用X射线粉末衍射仪（XRD）、透射电子显微镜（TEM）、红外光谱（IR）和振动样品磁强计（VSM）等手段对样品进行了表征,结果表明,样品为尖晶石型铁酸镉纳米粉体,其粒径大约为20—50nm,且具有超顺磁性。     

尖晶石型纳米铁酸镍的制备与磁性研究

以Fe（NO3）3·9H2O和Ni（NO3）2·6H2O为原料,用柠檬酸为还原剂,采用燃烧法制备了NiFe2O4纳米粉体,用X射线粉末衍射仪（XRD）、透射电子显微镜（TEM）、红外光谱（IR）和振动样品磁强计（VSM）等手段对样品进行了表征,结果表明,样品为立方晶系尖晶石铁酸镍纳米粉体,其粒径在20—40nm之间,具有超顺磁性,并探讨了焙烧温度、焙烧时间对样品磁性的影响。     

纳米晶ZnO可见发射机制的研究

利用化学沉淀法制备了纳米ZnO粉体,室温下测量了样品的光致发光谱(PL)、X射线衍射谱(XRD),给出了样品的透射电子显微照片(TEM).X射线衍射(XRD)的结果表明:纳米晶ZnO具有六角纤锌矿晶体结构,颗粒呈球形或椭球形.观察到二个荧光发射带,中心波长分别位于398 nm的紫带和510 nm的绿光带.发现随退火温度升高,粒径增大,紫带的峰值减弱、绿带的峰值增强.证实了纳米晶ZnO绿光可见发射带来自氧空位形成的施主和锌空位形成的受主之间的复合.     

Preparation and characterization of flaky FeSiAl composite magnetic powder core coated with MnZn ferrite

The flattening of FeSiAl soft magnetic powder was achieved by ball milling process, and MnZn/FeSiAl composite magnetic powder core was prepared by press molding. The effect of different coating amount of MnZn ferrite on the soft magnetic properties of FeSiAl was studied. At the same time, the optimal stress-relieving annealing temperature of the composite magnetic powder core is revealed. The results showed that the addition of MnZn ferrite affected the magnetic properties such as saturation magnetization (Ms), initial permeability (μi) and power loss (Pcm) of FeSiAl soft magnetic. With the increase of MnZn ferrite addition content, the saturation magnetization of composites decreased gradually, and the magnetic permeability increased first and then decreased, and the loss decreased first and then increased. When the addition content of MnZn ferrite was 5%, the permeability reached the maximum, which was 28.1% higher than that of the pure FeSiAl magnetic powder core under the same conditions. At the same time, the loss was the lowest, which was 13.3% lower than the pure FeSiAl powder core under the same conditions. When the annealing temperature is around 650 °C, the magnetic powder core has the largest magnetic permeability and the lowest loss.     

Superior values of the initial permeability for electrodeposited Ni–Co–P-BaFe12O19 composite films

In this research, we detected superior values of the initial magnetic permeability for electrodeposited Ni–Co–P-M-type BaFe₁₂O₁₉ (BaM) composite films as magnetic soft–hard composites with a large amount of entrapped BaM particles. Furthermore, the initial magnetic permeability of Ni–Co–P-BaM composite films is significantly large and is comparable with corresponding values of the excellent corresponding values for permalloys, Sendust, Co-based amorphous alloys, nanocrystalline (Fe-based) and commercially sintered MnZn ferrite cores. Therefore, Ni–Co–P-BaM composite films are very attractive for magnetic devices, such as magnetic inductors, transformers, and magnetic recording heads.     

Analysis of the complex permeability of monocrystalline MnZnFeII ferrite

A method of analysis is discussed by means of which the domain wall susceptibility and rotational susceptibility of monocrystalline MnZn ferrite can be distinguished. It is based upon a measurement of the frequency dependence of the disaccommodation occurring in the ferrite. From this analysis it appears that below 1 MHz the domain wall motion is the dominating magnetization process in MnZn ferrite, whereas above 3 MHz the rotational susceptibility prevails. Between 1 and 3 MHz, μ′ and μ″ are determined mainly by the rotational- and wall-susceptibility, respectively. Hence, when applied in magnetic video heads, the ferrite may generate electrical noise as a result of the dissipation accompanying the wall motion.     

Barium ferrite powders prepared by microwave-induced hydrothermal reaction and magnetic property

We have prepared barium ferrite particles by the microwave-induced hydrothermal method. The crystallization of the barium ferrite particles is promoted within a short time by microwave irradiation because the seeds of barium ferrite having large permeability are rapidly heated through the interaction of barium ferrite with the magnetic component of the microwaves. Crystals having unusually low thickness were obtained compared with the conventional hydrothermal method. The magnetic properties of barium ferrite particles are discussed.     

Combined effect of demagnetizing field and induced magnetic anisotropy on the magnetic properties of manganese-zinc ferrite composites

This work is devoted to the analysis of factors responsible for the high-frequency shift of the complex permeability (μ^?) dispersion region in polymer composites of manganese-zinc (MnZn) ferrite, as well as to the increase in their thermomagnetic stability. The magnetic spectra of the ferrite and its composites with polyurethane (MnZn-PU) and polyaniline (MnZn-PANI) are measured in the frequency range from 1 MHz to 3 GHz in a longitudinal magnetization field of up to 700 Ое and in the temperature interval from −20 °С to +150 °С. The approximation of the magnetic spectra by a model, which takes into account the role of domain wall motion and magnetization rotation, allows one to determine the specific contribution of resonance processes associated with domain wall motion and the natural ferromagnetic resonance to the μ^?. It is established that, at high frequencies, the μ^? of the MnZn ferrite is determined solely by magnetization rotation, which occurs in the region of natural ferromagnetic resonance when the ferrite is in the “single domain” state. In the polymer composites of the MnZn ferrite, the high-frequency permeability is also determined mainly by the magnetization rotation; however, up to high values of magnetizing fields, there is a contribution of domain wall motion, thus the “single domain” state in ferrite is not reached. The frequency and temperature dependence of μ^? in polymer composites are governed by demagnetizing field and the induced magnetic anisotropy. The contribution of the induced magnetic anisotropy is crucial for MnZn-PANI. It is attributed to the elastic stresses that arise due to the domain wall pinning by a polyaniline film adsorbed on the surface of the ferrite during in-situ polymerization.     

Dependence of microwave absorption properties on ferrite volume fraction in MnZn ferrite/rubber radar absorbing materials

We report the analysis of measurements of the complex magnetic permeability (μ_r) and dielectric permittivity (ε_r) spectra of a rubber radar absorbing material (RAM) with various MnZn ferrite volume fractions. The transmission/reflection measurements were carried out in a vector network analyzer. Optimum conditions for the maximum microwave absorption were determined by substituting the complex permeability and permittivity in the impedance matching equation. Both the MnZn ferrite content and the RAM thickness effects on the microwave absorption properties, in the frequency range of 2-18 GHz, were evaluated. The results show that the complex permeability and permittivity spectra of the RAM increase directly with the ferrite volume fraction. Reflection loss calculations by the impedance matching degree (reflection coefficient) show the dependence of this parameter on both thickness and composition of RAM.     

Interaction effects in magnetic oxide nanoparticle systems

The interaction effects in magnetic nanoparticle system were studied through a Monte Carlo simulation. The results of simulations were compared with two different magnetic systems, namely, iron oxide polymer nanocomposites prepared by polymerization over core and nanocrystalline cobalt ferrite thin films prepared by sol-gel process. The size of the particles in the nanocomposites were estimated to be ∼15 nm with very little agglomeration. The low values of the coercivity obtained from the hysteresis measurements performed confirm that the system is superparamagnetic. SEM studies showed the cobalt ferrite films to have a nanocrystalline character, with particle sizes in the nanometer range. Hysteresis measurements performed on the thin films coated on silicon do not give evidence of the superparamagnetic transition up to room temperature and the coercivity is found to increase with decreasing film thickness. Comparison with simulations indicate that the nanocomposites behave like a strongly interacting array where exchange interactions lead to high blocking temperatures, whereas the films are representative of a semi-infinite array of magnetic clusters with weak interactions and thickness-dependent magnetic properties.     

Surface modification of M-Ba-ferrite powders by polyaniline: Towards improving microwave electromagnetic response

A composite of polyaniline (PANI)-coated M-type hexagonal barium ferrite (M-Ba-ferrite) powder was prepared by an in situ polymerization of an aniline monomer in the presence of M-Ba-ferrite particles. The obtained composite was characterized by Fourier transform infrared spectra (FT-IR), X-ray diffraction (XRD) and transmission electron microscopy (TEM). The structure and microwave response properties were investigated. The continuous coverage of polyaniline has been produced on the platelet M-Ba-ferrite particle surface, and a core–shell structure has been formed. The results show that the coverage of polyaniline has a great influence on microwave response of M-Ba-ferrite particles. A polyaniline thin layer formed on the surface of a barium ferrite particle changes the character of frequency dispersion of microwave absorption. The results indicate the existence of an interaction at the interface of polyaniline macromolecule and barium ferrite particle, which influences the physical and chemical properties of the composite. The interaction and interfacial polarization are seen as important factors contributing to the influence on microwave response of the PANI-coated ferrite composite powders.     

Cobalt ferrite nanoparticles: The control of the particle size and surface state and their effects on magnetic properties

In order to improve the efficacy of magnetic fluid hyperthermia (MFH) mediators, we synthesised cobalt ferrite nanoparticles with different sizes (between 5 and 7 nm) via successive polyol synthesis. The static and dynamic magnetic properties of the prepared particles, dispersed in a solid matrix, were investigated in order to evaluate the possibility of applying cobalt ferrite as magnetic susceptors in MFH. The effect on magnetic properties coming from the surface anchoring of the model molecule cetyl phosphate, was also investigated.