共沉淀法制备Co掺杂ZnO的室温铁磁性的研究

利用共沉淀法并在5vol.%H₂/Ar气流中于300 ℃退火3 h,制备了Zn_1-xCo_xO稀磁半导体. 扫描电子微探针分析表明,对Co的名义组分分别为0.05,0.10,0.15的样品,其实际组分分别为x＝0.054, 0.100和0.159. X射线衍射表明, 主相为纤锌矿结构, x=0.100和 0.159的样品中含有CoO杂相. X射线光电子谱显示出Co有３种状态: 替代进入Z 关键词： 稀磁半导体 ZnO 共沉淀法 磁性来源     

多晶Si0.9654Mn0.0346:B薄膜的磁性研究

利用磁控溅射和快速热处理的方法制备了Mn,B共掺的多晶硅薄膜(Si_0.9654Mn_0.0346:B).磁性和结构研究发现薄膜有两个铁磁相.低温铁磁相来源于杂相Mn₄Si₇,高温铁磁相(居里温度T_C～250K)是由Mn原子掺杂进入Si晶格导致.晶化后的薄膜利用射频等离子体增强化学气相沉积系统(PECVD)进行短暂(4min)的氢化处理后发现,薄膜的微结构没有发生变化而饱和磁化强度却随着 关键词： 磁性半导体 硅 氢化     

Ti掺杂对α″-Fe16N2相稳定性的影响

研究了掺杂Ti对α″-Fe₁₆N₂相稳定性的影响，发现适量Ti掺杂有利于α″-Fe₁₆N₂相的形成．理论分析表明，掺杂适量Ti元素后含Ti的α″-(Fe,Ti)₁₆N₂相的生成焓降低，使α″相的稳定性提高，也使α″相更易制备．Ti浓度为3—15at％的(FeTi)-N薄膜具有高饱和磁化强度，μ₀M_s=2.3—2.5T． 关键词：     

Fe100－xPdx合金纳米线阵列的制备及其磁性研究

利用直流电沉积法在多孔阳极氧化铝模板中制备出了一系列Fe_100-xPd_x磁性纳米线阵列. Pd的增加使纳米线的总体磁性降低，各向异性和矫顽力也发生了较大的变化. 当Pd含量高达x=30时，纳米线仍有相当高的矫顽力(7.48 kA/m)和较明显的各向异性，但当Pd的含量增加到50%时，纳米线的易磁化方向由平行线的方向反转到垂直线的方向. 实验证明，这是由于在Fe₈₀Pd₂₀和Fe₇₀Pd₃₀中连续的磁性相在Fe₅₀Pd₅₀纳米线中变成了与非磁性相相互间隔的非连续片状结构. 片状磁性相的形状各向异性使易磁化方向转变到垂直纳米线轴的方向. 从生长动力学的角度对Fe₅₀Pd₅₀纳米线中这种片状的形成进行了解释. 关键词： 纳米线 电化学沉积 磁性     

NdFe10M2(M=Mo,Cr)渗C(N)化合物的结构和内禀磁性研究

本文采用气—固反应，将Ｃ、Ｎ原子渗入到ＮｄＦｅ₁₀Ｍ₂结构中的间隙位，不改变它们的ＴｈＭｎ₁₂型结构，进而研究了ＮｄＦｅ₁₀Ｍ_xZ_x（ｚ＝Ｃ，Ｎ）的内禀磁性，Ｃ，Ｎ原子对它们的磁性影响不尽相同，其中ＮｄＦｅ₁₀Ｍｏ₂Ｃ_0.8有单轴各向异性，磁晶各向异性场Ｈ_s＝１１６．０ｋＯｅ。最后对样品进行了穆斯堡尔谱测量，研究了它们的超精细场特性。 关键词：     

热处理对非晶态合金Nd4Fe96-xBx磁性的影响

本文研究了用单辊急冷方法制备的非晶态合金Nd₄Fe_96-xB_x的晶化,以及热处理对其硬磁性和相组成的影响,发现非晶态合金Nd₄Fe_96-xB_x的晶化温度比相同B含量的非晶态合金Fe_100-xB_x高120—190K,X射线衍射和热磁测量表明,15≤x≤25的样品晶化相是由Nd₂Fe₁₄B(T 关键词：     

静电纺丝法制备Bi2Fe4O9及其磁学性能的研究

采用静电纺丝法合成了纤维状的Bi₂Fe₄O₉前驱体,再对前驱体进行热处理得到了棒状的Bi₂Fe₄O₉.通过X射线衍射、扫描电子显微镜及透射电子显微镜表征了合成样品的物相及形貌特征.结果表明合成的样品为Bi₂Fe₄O₉单相,属于正交晶系;退火处理导致纤维状的前驱体转变为棒状的Bi₂Fe₄O₉.紫外-可见吸收光谱表明制备的Bi₂Fe₄O₉对光的吸收范围广,不仅对紫外光具有较强吸收,而且对可见光也有一定的吸收.通过振动样品磁强计测定Bi₂Fe₄O₉磁滞回线研究其磁学特性,相应的矫顽力H_C≈82 Oe（1 Oe=79.5775 A/m）,剥离顺磁信号后的剩磁M_r≈0.25 emu/g,研究发现Bi₂Fe₄O₉样品具有弱铁磁性,并且软磁性能有所提高.     

YTi(Fe1-xCox)11的磁性和穆斯堡尔谱的研究

YTi(Fe_1-xCo_x)₁₁在012型四方结构,居里温度随Co含量的增加而提高,本文为了揭示YTi(Fe_1-xCo_x)₁₁磁性与微观结构的联系,对这一系列化合物进行穆斯堡尔谱研究,在室温下,测量YTi(Fe_1-xCo_x)₁₁(其中x=0.0,0.2,0.4)的穆斯堡尔谱,最佳拟合结果证实在这种化合物中,Co原子优先占据j和f晶位,在所测样品中,超精细场在x=0.2处出现极值,这与YTi(Fe_1-xCo_x)₁₁饱和磁化强度测量结果相符合。并对YTi(Fe_1-xCo_x)₁₁,Y₂(Fe_1-xCo_x)₁₄和YTi(Fe_1-xCo_x)₁₁的穆斯堡尔谱的实验结果进行比较,分析在YTiFe₁₁中与Y₂Fe₁₄B中的3d电子能带结构的差异。 关键词：     

纳米超微晶Fe73.5Cu1Mo3Si13.5B9合金显微结构和磁性的研究

对纳米晶Fe_73.5Cu₁Mo₃Si_13.5B₉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：     

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：     

Electromagnetic and magnetic properties of magnetophotonic crystal based on opal matrix with Co and CoO nanoparticles

Magnetic properties of magnetophotonic crystals based on opal matrices have been studied as well as their electromagnetic properties in millimeter waveband. The particles of cobalt oxide are embedded into the inter-sphere voids of the matrix. After annealing in hydrogen the cobalt oxide particles transform to metallic cobalt. It has been shown that if antiferromagnetic cobalt oxide remains besides ferromagnetic cobalt, the low-temperature magnetic hysteresis loop is shifted along the field axis. Magnetic field influences essentially on the microwave transmission and reflection coefficients only after annealing in hydrogen that is if the ferromagnetic phase presents in the sample. The spectra of magnetic resonance and antiresonance are studied.     

Nickel–cobalt oxide/activated carbon composite electrodes for electrochemical capacitors

Nanostructured synthesis of nickel–cobalt oxide/activated carbon composite by adapting a co-precipitation protocol was revealed by transmission electron microscopy. X-ray diffraction analysis confirmed that nickel–cobalt oxide spinel phase was maintained in the pure and composite phases. Cyclic voltammetry, galvanostatic charge–discharge tests and ac impedance spectroscopy were employed to elucidate the electrochemical properties of the composite electrodes in 1.0 M KCl. The specific capacitance which was the sum of double-layer capacitance of the activated carbon and pseudocapacitance of the metal oxide increased with the composition of nickel–cobalt oxide before showing a decrement for heavily-loaded electrodes. Utilisation of nickel–cobalt oxide component in the composite with 50 wt. % loading displayed a capacitance value of ～59 F g^?1. The prepared composite electrodes exhibited good electrochemical stability.     

Cobalt Modification of Thin Rutile Films Magnetron-Sputtered in Vacuum

Using X-ray phase analysis, atomic force microscopy, and secondary ion mass-spectrometry, the phase formation and component distribution in a Co–TiO₂ film system have been investigated during magnetron sputtering of the metal on the oxide and subsequent vacuum annealing. It has been found that cobalt diffuses deep into titanium oxide to form complex oxides CoTi₂O₅ and CoTiO₃. A mechanism behind their formation at grain boundaries throughout the thickness of the TiO₂ film is suggested. It assumes the reactive diffusion of cobalt along grain boundaries in the oxide. A quantitative model of reactive interdiffusion in a bilayer polycrystalline metal–oxide film system with limited solubility of components has been developed. The individual diffusion coefficients of cobalt and titanium have been determined in the temperature interval 923–1073 K.

     

Structure and the magnetic and magneto-optical properties of Co-Sm-O nanogranular films

The magnetic properties and magneto-optical effects in nanocomposites based on Co-Sm-O films prepared through pulsed plasma sputtering of a SmCo₅ target are investigated. It is shown that, depending on the technological conditions and regimes of subsequent annealing, the films can have different structures from cobalt nanoparticles distributed in the dielectric samarium oxide matrix with a magnetic phase volume of more than 60% to a continuous polycrystalline cobalt film with embedded samarium oxide nanoparticles. The evolution of the spectra of the magneto-optical Kerr effect and the field dependences of the magnetization is studied as a function of the film structure.     

A novel strategy to synthesize cobalt hydroxide and Co3O4 nanowires

Cobalt hydroxide ultra fine nanowires were prepared by a facile hydrothermal route using hydrogen peroxide. This method provides a simple, low cost, and large-scale route to produce β-cobalt hydroxide nanowires with an average diameter of 5 nm and a length of ca. 10 μm, which show a predominant well-crystalline hexagonal brucite-like phase. Their thermal decomposition produced highly uniform nanowires of cobalt oxide (Co₃O₄) under temperature 500 °C in the presence of oxygen gas. The produced cobalt oxide was characterized by X-ray diffraction, transmission electronic microscopy, and selected-area electron diffraction. The results indicated that cobalt oxide nanowires with an average diameter of 10 nm and a length of ca. 600 nm have been formed, which show a predominant well-crystalline cubic face-centered like phase.     

Valence control of cobalt oxide thin films by annealing atmosphere

The cobalt oxide (CoO and Co₃O₄) thin films were successfully prepared using a spin-coating technique by a chemical solution method with CH₃OCH₂CH₂OH and Co(NO₃)₂·6H₂O as starting materials. The grayish cobalt oxide films had uniform crystalline grains with less than 50 nm in diameter. The phase structure is able to tailor by controlling the annealing atmosphere and temperature, in which Co₃O₄ thin film was obtained by annealing in air at 300-600, and N₂ at 300, and transferred to CoO thin film by raising annealing temperature in N₂. The fitted X-ray photoelectron spectroscopy (XPS) spectra of the Co2p electrons are distinguishable from different valence states of cobalt oxide especially for their satellite structure. The valence control of cobalt oxide thin films by annealing atmosphere contributes to the tailored optical absorption property.     

Faraday effect in nanogranular Co-Sm-O films

The Faraday effect (FE) was studied in Co-Sm-O composite films consisting of nanoparticles of metallic cobalt embedded in a samarium oxide dielectric matrix. The volume of the magnetic phase was ～60%. The FE spectral dependence for the condensates studied revealed a substantial change as compared to that for bulk cobalt samples, as well as for the films of nanocrystalline Co and CoSm films prepared in this study. An enhancement of the FE was also observed in the short-wavelength part of the optical spectrum.     

含钴玻璃熔制及其光谱曲线分析

用CoO着色可以生产蓝色玻璃,钴含量及玻璃配合料氧化还原性都容易造成玻璃光学指标的改变,使玻璃产生较大的色差。本文通过改变玻璃中钴的含量、氧化还原剂用量来熔制玻璃样片,然后用SP-1920分光光度计对玻璃样片进行光度指标分析。结果表明:着色剂的用量、配合料的氧化还原性、K2O的添加对玻璃光学指标有较大影响。     

Fabrication, sintering and electrical properties of cobalt oxide doped Gd0.1Ce0.9O2 − δ

Ceria-based electrolytes have been widely researched in intermediate-temperature solid oxide fuel cell (SOFC), which might be operated at 500~600 °C. Gd0.1Ce0.9O1.95(GDC10) powders were prepared by a modified chemical co-precipitation process with Gd(NO3)3 and Ce(NO3)3 as precursors, and ammonia and hydrogen peroxide as precipitants. The precursors of GDC10 were fired at 350 °C for 2 h, then the fluorite structure cerias were identified by X-ray diffraction. The powders are well crystallized, with the size about 5 nm and surface area of 148.3 m2/g. Loading 1mol% cobalt oxide as additive, the GDC10 were succeeded to densify at 950 °C by liquid phase sintering mechanism. The grain size of 1CoGDC10 is small, about 100 nm. The electrical conductivity of samples sintered at 950 °C is about 0.01S/cm at 600 °C. The existence of cobalt oxide and smaller grain size of 1CoGDC10 don't affect the electrical conductivity.     

An x-ray photoelectron spectroscopy study of the activated cobalt-molybdenum-alumina hydrodesulfurization catalysts

ESCA was used to monitor the chemical modification of a series of commercial cobalt-molybdenum-alumina hydrodesulfurization catalysts subjected to different reaction conditions. In the oxide form, the surface phase $\text{resembles}$ MoO₃ and CoAl₂O₄. Reduction and sulfiding using a 15:85 H₂S/H₂ mixture shifts the molybdenum peaks to the region of MoS₂. Part of the cobalt is apparently reduced and sulfided, but this species is susceptible to re-oxidation by moist air. The supported cobalt which is not changed by this treatment is interpreted as actually being CoAl₂O₄ formed by interaction of the dispersed material with the support during calcination. The presence of this aluminate phase seems to be important for the stability of the catalyst under the harsh conditions of industrial usage. Reduction of the oxide form by pure hydrogen leaves the molybdenum binding energy unchanged and shifts the cobalt peak to higher binding energy. This is interpreted as arising from a shift in reference level and it is concluded that the actual transformation