多波长线性回归分光光度法同时测定油中的铁、钴、镍

本文提出一种同时测定铁,钴,镍的新方法,即多波长线性回归分光光度法,利用铁与５－Ｂｒ－ＰＡＤＡＰ形成的络合物在７５０ｎｍ处吸收峰不受钴,镍干扰的特点,在７５０ｎｍ处于工作曲线法测定铁的含量,对于钴,镍在５５０－６００ｎｍ内采用多波长线性回归法测定。应用于合成样及油样中铁,钴,镍含量的测定,结果令人满意,回收率为９５．７％￣１０４．３％,相对标准偏差为１．４％￣３．８％。     

蓝宝石衬底上生长的Ga2+xO3-x薄膜的结构分析

利用卢瑟夫背散射/沟道技术和金属有机化学气相沉积方法, 对蓝宝石衬底上 在不同温度、压强下生长的Ga_2+xO_3-x薄膜进行结构和结晶品质的测量与分析; 并结合高分辨X射线衍射分析技术, 通过对其对称(402)面的θ–2θ及ω扫描, 确定了其结构类型及结晶品质. 实验表明: 在相同的生长温度(500 ℃)下, 结晶品质随压强的下降而变好, 生长压强为15 Torr (1 Torr=133.322 Pa)的样品其结晶品质最好, 沿轴入射之比χ_min值为14.5%; 在相同的生长压强(15 Torr)下, 结晶品质受生长温度的影响不大, 所以, 生长温度不是改变结晶品质的主要因素; 此外, 在相同的生长条件下制备的样品, 分别经过700, 800和900 ℃退火后, 其结晶品质随退火温度的变化而变化. 退火温度为800 ℃的样品的结晶品质最好, χ_min值为11.1%; 当退火温度达到900 ℃时, 样品部分分解; 经热处理的样品其X射线衍射谱中有一个强的Ga₂O₃ (402)面衍射峰, 其半峰全宽为0.5°, 表明该Ga₂O₃外延膜是(402)择优取向. 关键词： 氧化镓 卢瑟夫背散射 X射线衍射 结晶品质     

双波长标准加入法同时测定钴镍合金镀液中的钴(Ⅱ)和镍(Ⅱ)

在 p H5 .0的乙酸 -乙酸钠缓冲溶液和聚乙烯醇体系中 ,钴 ( )和镍 ( )可与 PAN试剂形成稳定的络合物。以钴 ( )的 5 80 nm和 6 2 6 nm为测定波长对 ,镍作标准加入组分 ,双波长标准加入法可同时测定试样中钴、镍的含量。镍在 0— 15 μg/2 5 m L,钴在 0— 10 μg/2 5 m L范围内遵从比耳定律。对镀液样品进行测定 ,镍、钴的相对标准偏差 (n=6 )分别 <0 .82 %和 <1.2 %。     

钨粉的平面动载压实

 本文研究了粒度为3 μm与20 μm两种钨粉的平面动载压实。证明粒度较小的钨粉在压实后分层严重，中层疏松。要得到良好的压实件，钨粉要有一定值以上的粒度，碰撞速度要在1 100 m/s以上，钨粒中要配以一定量的钴、镍、铁粘结相。这些能用Carroll和Holt的球壳模型作的数值模拟计算清楚说明。     

不同催化剂对热解法制备CNx纳米管的影响

利用铁、钴、镍以及二茂铁为催化剂在高温下热解乙二胺制备CNx纳米管,研究了不同催化剂对CNx纳米管的形貌、结构及产量的影响,并对其催化机理进行了初步讨论.二茂铁和铁催化都能制备出“竹节状”结构的CNx纳米管,但产量较低.钴催化生成CNx纳米管多弯曲,管壁多褶皱,产量较高.镍催化只生成了直径500nm左右的螺旋管.拉曼光谱研究进一步表明,二茂铁催化生成“竹节状”结构CNx纳米管由于氮的掺杂程度相对较高而结晶有序度较低.     

爆轰合成碳包覆钴、镍磁性纳米颗粒的探索

 介绍了爆轰法合成碳包覆钴、镍纳米磁性颗粒研究的初步结果。以黑索今炸药为主体,加入钴、镍金属硝酸盐与有机碳源材料,在爆炸容器中氮气保护下用导爆管雷管引爆,成功地合成了碳包覆钴、镍纳米磁性颗粒。为了探求爆轰固体产物的形貌特征及性能,分别采用了TEM、XRD、VSM等测试手段对其进行表征。实验结果表明,爆轰产物中主要含有碳包覆纳米钴、纳米镍磁性颗粒,成球体或者椭球体,具有完好的核壳结构形貌。合成的碳包覆钴颗粒分布在30~50 nm之间,碳包覆的镍颗粒分布在25~60 nm之间,外层碳壳层主要由无定形碳和石墨构成。磁性测试表明,所得碳包金属钴、镍颗粒在室温下具有良好的软磁特性。     

过渡金属原子掺杂的锯齿型磷烯纳米带的磁电子学特性

利用基于密度泛函理论的第一性原理方法,研究了掺杂铁、钴和镍原子的锯齿型磷烯纳米带(ZPNR)的磁电子学特性.研究表明,掺杂和未掺杂ZPNR的结构都是稳定的.当处于非磁态时,未掺杂和掺杂钴原子的ZPNR为半导体,而掺杂铁或者镍原子的ZPNR为金属.自旋极化计算表明,未掺杂和掺杂钴原子的ZPNR无磁性,而掺杂铁或者镍原子的ZPNR有磁性,但只能表现出铁磁性.处于铁磁态时,掺杂铁原子的ZPNR为磁性半导体,而掺杂镍原子的ZPNR为磁性半金属.掺杂铁或者镍原子的ZPNR的磁性主要由杂质原子贡献,产生磁性的原因则是在ZPNR中存在未配对电子.掺杂位置对ZPNR的磁电子学特性有一定的影响.该研究对于发展基于磷烯纳米带的纳米电子器件具有重要意义.     

彩色金刚石中过渡金属离子的谱学研究

过渡金属镍、钴和铁是高温高压法合成金刚石的常用触媒,已有研究表明：采用镍、钴作触媒所合成的金刚石中存在镍、钴离子,部分天然金刚石含有镍离子;镍、钴离子以替代方式或间隙形式进入金刚石的晶格,并能与杂质氮形成复合体。为了探寻彩色金刚石中过渡金属离子存在的谱学标志,确定镍、钴离子在彩色金刚石中的赋存状态,文章对6颗彩色天然与合成金刚石进行了扫描电镜-能谱、显微红外光谱、光致发光谱、电子顺磁共振谱(EPR)等测试研究。结果表明天然与合成的样品都具有与镍、钴有关的发光中心与EPR结构：包括西澳的蓝灰色天然金刚石中与镍有关的884.6 nm等发光中心,以及天然变色金刚石中与钴有关的发光中心。对各种谱学测试结果的综合分析,得出样品中存在镍、钴离子并与杂质氮形成各种Ni-N或Co-N复合体的结论,其中在天然金刚石中发现钴离子在该领域研究中尚属首次。     

ICP-AES同时测定镍锰钴硅铁铌硼合金中钴、铌、铁和硼

用全谱直读ICP-AES分析技术,对试样溶解方法、元素分析谱线、共存元素干扰、背景校正、仪器分析参数等进行了研究,综合确定了最佳实验条件。将镍锰钴硅铁铌硼合金试样用硝酸、氢氟酸溶解,ICP-AES直接测定钴、铌、铁、硼。测定范围为：Co0.5%—12%、Fe0.1%—3%、Nb0.1%—5%、B0.05%—1.0%。加标回收率为96.6%—103.7%,相对标准偏差为0.37%—4.56%。方法简便、快速、准确。     

显色剂1-(2-苯并噻唑)-3-(5,7-二溴-8-喹啉)-三氮烯的合成及与钴的显色反应

合成了新显色剂 1- (2 -苯并噻唑 ) - 3- (5 ,7-二溴 - 8-喹啉 ) -三氮烯 (BTDBQT) ,并研究了在阳离子表面活性剂存在下与钴的显色反应。在 p H9.5— 10 .5的硼酸盐缓冲介质中 ,钴与该试剂形成 1∶ 2的蓝色铬合物 ,其最大吸收波长在 6 42 nm处 ,表观摩尔吸光系数为 1.0 5× 10 5L· mol-1·cm-1,钴 ( )的浓度在0— 2 4 0 μg/ L范围内符合比耳定律。显色反应具有良好的选择性 ,常见离子除铜、镍外 ,基本不干扰测定。已应用于维生素 B12 和水系沉积物中微量钴的测定     

Magnetic impedance of structured film meanders in the presence of magnetic micro- and nanoparticles

The magnetic impedance (MI) of film elements in the form of meanders with a [Fe19Ni81]/Cu]₄/Fe19Ni81/Cu/[Fe19Ni81/Cu]₄/Fe19Ni81 layered structure and variable geometry is studied. For the best meanders (having a maximal MI of up to 125% and an MI maximal sensitivity of about 30%/Oe), the influence of stray magnetic fields is determined. The stray fields are produced by spherical iron particles 500 μm in diameter and ferrofluids containing iron oxide nanoparticles. The feasibility of detecting intricately configured stray fields from a set of ferromagnetic spheres arranged on the surface of an MI element is demonstrated. The sensitivity of film meander MI elements to nonuniform external magnetic fields is simulated. The results of this work may be helpful in developing special-purpose magnetic sensors intended for micropositioning, nondestructive testing, and biomagnetic detection.     

Properties of three-dimensional composites based on opal matrices and magnetic nanoparticles

Three-dimensional nanocomposites consisting of an opal matrix and a metal have been prepared by the interaction of salts and oxides of different elements (Ni, Co, Fe, etc.) embedded in an opal matrix with isopropanol in the range of supercritical state parameters of the alcohol. According to X-ray powder diffraction analysis and transmission electron microscopy data, the composites consist of an X-ray amorphous opal matrix with pores filled by nanoparticles of Co (or CoO _x ), metallic Ni, or Fe₃O₄ with a magnetite structure of various morphology. The sizes of the nanoparticles do not exceed the diameter of the pores in the opal matrix. A complex investigation of the nanocomposites has been performed using the electron magnetic resonance and vibrating magnetometry methods. All the studied samples at room temperature exhibit a ferromagnetic behavior. The coercive force of the samples lies in the range from 150 Oe for iron-containing nanocomposites to 565 Oe for cobalt-containing nanocomposites.     

Magnetic Properties of Fe/Ni and Fe/Co Multilayer Thin Films

In this work, the magnetic and transport properties of Fe/SiO₂/Ni and Fe/SiO₂/Co multilayers grown on Si/SiO₂ substrates have been studied. The samples have been prepared by two-stage deposition process. In the first stage, Fe layer and SiO₂ interlayer of both samples are grown by ion beam deposition technique at room temperature. Then the samples are taken out to ambient atmosphere and loaded into a pulse laser deposition (PLD) chamber. Prior to the deposition of top layer, the samples are cleaned by annealing at 150 °C. In the second stage, Ni (or Co) layer is prepared by PLD technique at room temperature. The thickness of deposited layers has been measured by Rutherford back scattering (RBS). Magnetic properties of ferromagnetic bilayers have been investigated by room-temperature ferromagnetic resonance (FMR) and vibrating sample magnetometer (VSM) techniques. Standard four-point magneto-transport measurements at various temperatures have been performed. Two-step switching in the in-plane hysteresis loops of Fe/SiO₂/Ni and Fe/SiO₂/Co samples is observed. A crossing in the middle of hysteresis loops of both samples points to a weak antiferromagnetic interaction between the magnetic layers of the stacks. Saturation magnetization values have been obtained from the VSM measurements of samples with DC magnetic field perpendicular to the films surface. Magneto-transport measurements have shown the predominant contribution of anisotropic magnetic resistance both at room and low temperatures. FMR studies of Fe/SiO₂/Ni and Fe/SiO₂/Co samples have revealed additional non-uniform (surface and bulk SWR) modes, which behavior has been explained in the framework of the surface inhomogeneity model. An origin of the antiferromagnetic interaction has been discussed.     

Structural and magnetic properties of transition metal oxide/metal bilayers prepared by in situ oxidation

Metal oxide/metal bilayers have been prepared by in situ oxidation. Ultrathin layers with antiferromagnetic properties are formed at room temperature by controlled in situ exposure of clean Fe, Co and Ni layers to pure oxygen gas. X-ray diffraction, Auger electron spectroscopy and transmisson electron microscopy have been applied to provide a detailed analysis of the layered structure. The magnetic properties of these antiferromagnetic/ferromagnetic bilayers are characterized by an interfacial coupling (exchange bias) which drastically varies with the type of antiferromagnetic material.     

Matrix embedded cobalt-carbon nano-cluster magnets: behavior as room temperature single domain magnets

A new type of Co-C nanoparticles is synthesized from CH₂Cl₂ solution of Co₄(CO)_{1 2} by heating up to 210 ^°C in a closed vessel. Transmission electron microscope (TEM) and electron energy loss spectroscopy (EELS) observation show that the particles are embedded in amorphous carbon and their average size is 12 nm. The radial structure function obtained from the extended X-ray absorption fine structure (EXAFS) of the Co K-edge absorption of the Co-C nanoparticles provides a Co-C average distance of 2.08 Å and the Co-Co distances of 3.18 Å and 3.9 (±0.2) Å. The particles exhibit the magnetic hysteresis curve with a coercive force of 200 Oe at 20 K and 260 Oe at 300 K. The temperature dependence of the magnetic susceptibility measured under zero-field cooling and 10 Oe field cooling conditions exhibits the behavior characteristic of a set of single magnetic domain nanomagnets in an amorphous carbon matrix.     

Magnetic stripe domains in coupled magnetic sandwiches

Magnetic stripe domains in the spin reorientation transition region are investigated in (Fe/Ni)/Cu(001) and Co/Cu/(Fe/Ni)/Cu(001) using photoemission electron microscopy. For (Fe/Ni)/Cu(001), the stripe domain width decreases exponentially as the Fe/Ni film approaches the spin reorientation transition point. For Co/Cu/(Fe/Ni)/Cu(001), the Fe/Ni stripe orientation is aligned with the Co in-plane magnetization, and the stripe domain width decreases exponentially with increasing the interlayer coupling between the Fe/Ni and Co films. By considering magnetic stripes within an in-plane magnetic field, we reveal a universal dependence of the stripe domain width on the magnetic anisotropy and on the interlayer coupling.     

Structure and magnetic properties of the oxide layers on iron ultrafine particles

5 . The γ-Fe particles, because of their paramagnetic nature, are very convenient for investigation on the attributes of iron oxide layers formed on the particle surfaces. Structures, morphologies and magnetic properties of the oxide layers covering the iron ultrafine particles have been studied using transmission electron microscopy observation, magnetic property measurement, X-ray diffraction and annealing treatment. Convincing evidences established that the iron oxide layers are not continuous and consist of very fine crystallites, and that these layers are non-ferromagnetic and have no contribution to the saturation magnetization of the iron particles. The iron oxide layers formed at room temperature was determined to be Fe₃O₄. Additionally, a brief annealing of the iron particles in air were performed to examine magnetic properties of the formed iron oxide layers and ultrafine oxide particles. Received: 30 April 1996/Accepted: 5 November 1996     

Magnetic structure of critical Fe-Ni alloys as derived from Arrott plots and Mössbauer spectra

New evidence of magnetic phase transition brought about by an external magnetic field acting on critical composition bulk Fe-Ni alloys was found by using iron-nickel alloys containing 30 wt% Ni and 31.3 wt% Ni, respectively (balance Fe). The split in the central peak of Mössbauer spectrum of the Fe-Ni alloy containing 29.7 wt% Ni, at its Curie temperature in a weak external magnetic field of 3100 Oe, is a conclusive evidence of its superparamagnetic structure.     

Magnetic properties of DNA-templated Co/Cu naonoparticle chains

<正>According to ultraviolet(UV)-vis absorption spectra recorded in the DNA metallization process,DNA-templated Co/Cu binary nanoparticle chains are fabricated by incubating genome DNA of paralichthys olivaceus muscle in CoCl_2 and CuCl_2 mixture solution for 20 hours and reducing the complex for 2 hours.Transmission electron microscopy observation indicates that Co and Cu nanoparticles with 20 nm in diameter were randomly dispersed on the DNA template. The superconducting quantum interference device(SQUID) measurements display that the magnetic interaction between cobalt particles is greatly decreased by the copper particle.With increasing copper content,the coercivity of the systems enhance from 9 Oe to 100 Oe(1 Oe=79.5775 A/m).     

磁场在水热制粉和固相制陶中的应用

本文介绍磁场在水热体系合成粉体以及在固相陶瓷块体织构研究中的应用.水热体系中,磁场引导合成的粉体主要有：Co,Ni等金属粉体,还有Fe3O4,BaFe12O19等铁氧体粉体.固相织构的陶瓷块体有：铁电压电材料,铁氧体磁性材料（包括尖晶石型,石榴石型和磁铅晶石型）,还有其他功能陶瓷如α-Al2O3.由于磁场的引导,这些材料都有沿易磁化晶体方向择优生长的特性,并表现出各自优异的性能.