包钴型γ-Fe2O3磁粉的穆斯堡尔谱研究

用穆斯堡尔谱学并配合宏观手段,研究不同工艺条件下的包钴型γ-Fe₂O₃磁粉以及扩样试验磁粉,将不同工艺下磁粉矫顽力的变化与微观结构联系起来。 关键词：     

包钴型r-Fe2O3磁粉各向异性研究

包钴型γ-Fe₂O₃磁粉的矫顽力可比原γ-Fe₂O₃磁粉提高8000—32000A/m。木文研究探讨了两种包钴型γ-Fe₂O₃磁粉(包钴γ-Fe₂O₃和包钴包亚铁γ-Fe₂O₃)的单轴各向异性的起源和矫顽力增大的机制。包钴γ-Fe₂O₃磁粉矫顽力 关键词：     

包钴型γ-Fe_2O_3磁粉矫顽力的研究

包钴型γ-Fe_2O_3磁粉分为包钴γ-Fe_2O_3(简记为Co-γ-Fe_2O_3)和包钴包亚铁γ-Fe_2O_3(简记为 CoFe-γ-Fe_2O_3)两种,它们的矫顽力可比γ-Fe_2O_3磁粉的提高100至400Oe左右,本工作对这两种磁粉矫顽力增大的原因作了探讨,认为它们矫顽力增大的机制不同:CO-γ-Fe_2O_3矫顽力增大是由于表面包覆一层Co(OH)_2使表面各向异性增大,而CoFe-γ-Fe_2O_3则是由于表面包覆的是钴铁氧体,γ-Fe_2O_3与钴铁氧体之间发生耦合作用,使矫顽力增大。     

γ-Fe2O3中的氢含量

利用热中子透射法测定γ-Fe₂O₃的氢含量。利用差热分析、磁分析以及穆斯堡尔效应研究γ-Fe₂O₃的相变,实验结果表明在γ-Fe₂O₃结构中确实含有一定量的氢,当γ-Fe₂O₃结构中的阳离子空位被H¹⁺,Co²⁺,Si⁴⁺,P⁵⁺等离子占据时,将 关键词：     

包钴铁氧体型γ-Fe2O3磁粉穆斯堡尔效应的研究

包钴铁氧体型,γ-Fe₂O₃磁粉(简记为CoFe-γ-Fe₂O₃)是针状γ-Fe₂O₃磁粉与Co⁺⁺和Fe⁺⁺溶液起反应,在每个针状颗粒上包覆了一层钴铁氧体固溶体。经此种方法处理后的γ-Fe₂O₃磁粉的矫顽力及其它磁特性有较大的提高。如矫顽力由原来415Oe增加到715Oe;剩磁和矫顽力随时间及温度变化小等。我们利用穆斯堡尔效应并配合其它研究手段进行了研究,认为:CoFe-γ-Fe₂O₃磁粉矫顽力的提高,主要是由于γ-Fe₂O₃磁粉表面包覆了一层钴铁氧体固溶体,γ-Fe₂O₃与钴铁氧体固溶体之间发生磁耦合作用之故。 关键词：     

Co处理的γ-Fe2O3薄膜的界面研究

本文中对CoO与Fe₂O₃的界面进行了研究,结果表明,简单的CoO-γ-Fe₂O₃界面对于磁性能基本无影响。分析表明,“复杂的扩散界面”不大可能象以往认为的那样是矫顽力增长的主要原因。矫顽力的增长可能是由掺Co造成的一种体效应而不是界面效应。 关键词：     

包钴型γ—Fe_2O_3磁粉矫顽力增大原因的探讨

针状γ-Fe_2O_3磁粉与Co~(++)和Fe~(++)溶液或Co(OH)_2起反应,在每颗颗粒上包上了一层Co铁氧体。经这样处理后的γ-Fe_2O_3磁粉的矫顽力可由原来的420Oe增大到770Oe左右。研究了这种磁粉的矫顽力H_c随磁粉密度以及温度的变化等,认为这种磁粉矫顽力增大的原因是由于增加了磁粉的表面各向异性所致     

磁载光催化剂ZnO/ SiO2/γ-Fe2O3的光催化性能

本文采用液相沉积法制备出了纳米SiO2/γ-Fe2O3复合粒子,在其表面负载ZnO, 从而得到了易于磁性固液分离的磁载光催化剂ZnO/SiO2/γ-Fe2O3, 并通过XRD和TEM等测试技术对样品进行了表征。以可溶性染料亚甲基兰等为降解对象, 研究了磁载光催化剂ZnO/SiO2/γ-Fe2O3在紫外光下的光催化活性。结果表明, 在γ-Fe2O3和ZnO之间包覆一层无定形SiO2可使催化剂降佳率由20.76%提高到95.63%,并且该磁载光催化剂对染料有较好的降解效果, 在三次循环使用后仍能保持较好的光催化性能.     

Co淀积到γ-Fe2O3表面的光电发射谱研究

在γ-Fe₂O₃表面蒸镀不同厚度Co,观察到低Co覆盖度,Co具有很大活力与O₂结合,而使Fe还原.在θ=0.2—0.8时,表面上形成类CoFe₂O₄.Co覆盖度进一步增加,Fe在表面偏析,Co开始形成第二层,破坏了形成这种氧化物的条件.因此,这种铁钴氧化物与单层或亚单层包钴磁粉磁性的改善可能有密切关系. 关键词：     

Exchange bias behavior of monodisperse Fe3O4/γ-Fe2O3 core/shell nanoparticles

We have carried out systematic studies on well-characterized monodisperse Fe₃O₄/γ-Fe₂O₃ core/shell nanoparticles of 2-30 nm having a very narrow size distribution and possessing a uniquely mono-layer of surface γ-Fe₂O₃. This unique core-shell structure, probably having a disordered magnetic surface state, leads us to three key observations of unusual magnetic properties: i) a very large magnetic exchange anisotropy reaching over 7 × 10⁶ erg/cm³ for the smaller particles, ii) exchange bias behavior in the magnetization data of the core/shell Fe₃O₄/γ-Fe₂O₃ nanoparticles, and iii) the temperature dependence of the coercive field following an unusual exponential behavior.     

Pressure induced phase transition of nanocrystalline and bulk maghemite (γ-Fe2O3) to hematite (α-Fe2O3)

Phase transition and bulk moduli of bulk and nanocrystalline γ-Fe₂O₃ were studied using synchrotron X-ray diffraction under high pressure. Contrary to most other nanomaterials, nanocrystalline γ-Fe₂O₃ begins to transform into α-Fe₂O₃ at the same pressure as bulk γ-Fe₂O₃, which is caused by a special structure of γ-Fe₂O₃, in which there exist vacancies of crystal. It is believed that phase transition starts from a certain site of vacancy because of the stress concentration at vacancy sites. Compared to bulk material, nanocrystalline γ-Fe₂O₃ has a larger bulk modulus, which is ascribed to the large ratio of surface to volume.     

表面效应对γ-Fe2O3微粉饱和磁化强度的影响

我们制备了直径为80—700A的γ-Fe₂O₃微粉,测量了它的比饱和磁化强度σ_s和比表面积S_a,得出经验公式:σ_s(s=σ_s(∞)(1—aS_a)。假定微粉由两部分组成:第一部分是表面层,在磁场的作用下,它的磁矩只能转到与磁场成某个角度;第二部分是内部,它的磁矩可以转到磁场的方向。从这个简单的模型出发,上述的经验公式可以得到较好的解释。 关键词：     

超细颗粒γ-Fe2O3微粉包钴前后的各向异性

本工作利用穆斯堡尔谱并配合其它研究手段,测量了超细γ-Fe₂O₃微粉在包钴和不包钴两种情况下的各向异性常数K;观察到前者比后者的各向异性常数K增加30％左右。对普通针状包钴型γ-Fe₂O₃磁粉矫顽力增大的原因提供了进一步的说明。 关键词：     

Magnetic and microwave absorbing properties of polyaniline/γ-Fe2O3 nanocomposite

The conducting protonated polyaniline (ES)/γ-Fe₂O₃ nanocomposite with the different γ-Fe₂O₃ content were synthesized by in-situ polymerization. Its morphology, microstructure, DC conductivity and magnetic properties of samples were characterized by transmission electron microscopy (TEM), Fourier transform infrared spectroscopy (FTIR), four-wire-technique, and vibrating sample magnetometer (VSM), respectively. The microwave absorbing properties of the nanocomposite powders dispersing in wax coating with the coating thickness of 2 mm were investigated using a vector network analyzers in the frequency range of 7–18 GHz. The pure ES has shown the absorption band with a maximum absorption at approximately 16 GHz and a width (defined as frequency difference between points where the absorption is more than 8 dB) of 3.24 GHz, when 10% γ-Fe₂O₃ by weight is incorporated , the width is broadened to 4.13 GHz and some other absorption bands appear in the range of 7–13 GHz. The parameter dielectric loss tan δ_e (=ε″/ε′) in the 7–18 GHz is found to decrease with increasing γ-Fe₂O₃ contents with 10%, 20%, 30%, respectively, but magnetic loss tan δ_m (=μ″/μ′) increases with increasing γ-Fe₂O₃ contents. The results show that moderate content of γ-Fe₂O₃ nanoparticles embedded in protonated polyaniline matrix may create advanced microwave absorption properties due to simultaneous adjusting of dielectric loss and magnetic loss.     

包钴型r_Fe_2_O_3磁粉矫顽力增大原因的探讨

针状r_Fe_2_O_3 磁粉与Co++ 和Fe++ 溶液或Co(OH)_2_起反应, 在每颗颗粒上包上了一层Co 铁氧体.经这样处理后的r_Fe_2_O_3 磁粉的矫顽力可由原来的420 Oe增大到770 Oe左右.研究了这种磁粉的矫顽力Hc随磁粉密度以及温度的变化等, 认为这种磁粉矫顽力增大的原因是由于增加了磁粉的表面各向异性所致. 关键词：     

光解水α-Fe2O3电极表面的研究

本文利用Ar⁺轰击正分的α-Fe₂O₃表面,证明了轰击后的表面呈类FeO性质,存在Fe⁺⁺。提出了由于表面Fe⁺⁺的3d电子的催化作用,Fe⁺⁺能把吸附在它上面的H₂O先分解成OH-和H⁺,因而有助于提高光解水的效率的看法。用UPS和XPS等技术证实了类FeO表面吸附水后存在OH^-,确认Fe^{++关键词：}     

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     

The study of novel Fe3O4@γ-Fe2O3 core/shell nanomaterials with improved properties

The surface structure of the iron oxide nanoparticles obtained by the co-precipitation method has been investigated, and a thin layer of α-FeOOH absorbed on surface of the nanoparticle is confirmed by analyses of Fourier transform infrared (FTIR), X-ray photoelectron spectra (XPS) and surface photovoltage spectroscopy (SPS). After annealed at 400 °C, the α-FeOOH can be converted to γ-Fe₂O₃. The simple-annealed procedure resulted in the formation of Fe₃O₄@γ-Fe₂O₃ core/shell structure with improved stability and a higher magnetic saturation value, and also the simple method can be used to obtain core/shell structure in other similar system.     

Rheological properties of a γ-Fe2O3 paraffin-based ferrofluid

A stable γ-Fe₂O₃ paraffin-based ferrofluid was prepared via high energy milling. The magnetic particles were characterized using X-ray diffraction, dynamic light scattering and vibrating sample magnetometer techniques. The rheological properties of the ferrofluid were studied using a standard rotating rheometer. The magnetoviscous effect and thixotropy in the ferrofluid were studied. The formation and destruction of magnetically induced structures and the interactions of nanoparticles and aggregates are discussed.     

Relaxation structure analysis of Li inserted γ-Fe2O3

γ-Fe₂O₃ has a spinel structure with cation vacancy and is expected to perform as a favorable electrode material for secondary lithium-ion battery. When lithium is inserted electrochemically into γ-Fe₂O₃, prolonged potential change is observed after the insertion. In this study, we inserted various amount of Li into γ-Fe₂O₃ (x = 0.66, 1.1, 1.5 in terms of Li_XFe₂O₃), then made the circuit open, measured X-ray diffraction (XRD) patterns at various elapsed time, and analyzed the crystal structure change of γ-Fe₂O₃ with time by the Rietveld method. The X-ray Rietveld analysis revealed that the iron occupancy of 8a site decreased and that of 16c site increased with lithium insertion process and after lithium insertion, the iron occupancy of 8a site increased and that of 16c site decreased gradually with relaxation time. It is indicated that lithium prefer 8a site to occupy kinetically, on the other hand, prefer 16c site thermodynamically.