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：     

大面积α-Fe2O3纳米线及纳米带阵列的制备研究

以铁箔为原材料和基片,通过控制热氧化过程中的宏观实验条件(载气流量及其组分、压强、温度分布和反应时间等),实现了α-Fe₂O₃一维纳米结构的可控生长,获得了大面积(10mm×10mm)、单分散性好、沿［110］方向生长的α-Fe₂O₃纳米带或纳米线阵列. 对不同宏观实验条件下所制备的样品进行形貌和晶格结构表征和分析,认为热氧化过程中α-Fe₂O₃一维纳米结构的生长遵循类似气- 关键词： 2O₃')" href="#">α-Fe₂O₃ 一维纳米结构 热氧化法     

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：     

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：     

包钴对α-Fe2O3粉末Morin相变的影响

用穆斯堡尔谱,磁性测量,中子衍射和X射线光电子能谱(XPS)等方法对纯的和包钴α-Fe₂O₃粉末Morin相变的影响以及有关性质进行了研究,发现包钴会使α-Fe₂O₃的Morin温度降低,相变温度的区域扩大,矫顽力明显增大,3d能带变化,假设包钴可使α-Fe₂O₃的单离子各向异性常数K_FS下降来解释上述实验结果。 关键词：     

AgI(α-Fe2O3)复合离子导体相转变温度相互影响的研究

通过测量AgI(α-Fe₂O₃)复合离子导体的直流和交流电导率,发现α-Fe₂O₃的Morin转变温度随着AgI含量的增加而降低,电导率测量的结果与磁化率测量和M?ssbauer谱测量结果定性的符合。α-Fe₂O₃也使AgI的α→β相转变温度显著下降。结果表明复合离子导体二相材料各自存在的相转变温度彼此产生影响。 关键词：     

磁性隧道结Ni80Fe20/Al2O3/Co的研究

用等离子体氧化形成中间绝缘层的方法可重复制备出具有隧道磁电阻（TMR)效应的Ni₈₀Fe₂₀/Al₂O₃/Co磁性隧道结.光透射谱等实验结果表明等离子体氧化能可控制地制备较致密的Al₂O₃绝缘层.样品的TMR比值在室温下最高可达6.0％,反转场可低于800A/m,相应的平台宽度约为2400A/m.结电阻R_j的变化范围从百欧到几百千欧,并且TMR比值随零磁场结偏压增大单调减小. 关键词：     

(Ni0.8Zn0.2Fe2O4)epoxy-PZT双层膜中的磁电效应

讨论了Ni_0.8Zn_0.2Fe₂O₄ (NZFO)与锆钛酸铅(PZT)的双层膜结构样品的磁电(ME)效应.NZFO粉料由溶胶-凝胶法制成，再经900℃热压，并高温烧结.在该双层膜中测量到了很强的磁电相互作用.发现横向的磁电效应比纵向效应大一个数量级，并且随NZFO烧结温度的提高而增加.当烧结温度从950℃上升到1380℃时，横向ME电压系数(α_E)的最大值变化范围为25.6 mV Am^-2≤α_E≤199.6 mV Am^-2.理论分析显示NZFO-PZT双层膜样品中ME效应源于NZFO与PZT之间相对良好的磁电耦合. 关键词： 镍铁氧体 PZT 热压法 ME效应     

纳米结构Zn_xFe_(3-x)O_4-α-Fe_2O_3多晶材料中的巨隧道磁电阻效应

在具有纳米绝缘层的多晶锌铁氧体体系中 ,当晶界为α Fe2 O3纳米量级 ( 6— 7nm)的绝缘层时 ,则构成 (ZnxFe3-xO4 ) α Fe2 O3非均匀体 ,高分辨电子显微镜已证实了这种微结构 ,该体系在 0 .5T磁场、4 .2K温度下 ,磁电阻效应可达12 80 % ,3 0 0℃下为 15 8% .     

α-Fe2O3单离子磁晶各向异性的计算及Morin转变的解释

本文根据晶场理论计算了α-Fe₂O₃的单离子磁晶各向异性。采用点电荷模型,计及近邻及次近邻对晶场的贡献,并考虑到近邻O^2-离子对次近邻Fe³⁺离子的电屏蔽效应,在六级微扰近似下,得到单离子各向异性场H_si=102.3×10²Oe。这一结果结合Artman等人对磁偶极各向异性的计算,导出了α-Fe₂O₃的Morin转变温度T _关键词：     

Inverse TMR in a nominally symmetric CoFe/AlOx/CoFe junction induced by interfacial Fe3O4 investigated by STEM-EELS

We have found inverse tunneling magnetoresistance (TMR) with a non-symmetric bias voltage dependence in a nominally symmetric Si (001)/Ag/CoFe/AlO_x/CoFe/IrMn/Ag magnetic tunnel junction after field cooling. The O K edge fine structure extracted from electron energy loss spectroscopy spectrum images taken at the interfaces of junctions with inverse TMR shows a thin, discontinuous Fe₃O₄ layer at the CoFe/AlO_x interfaces. The Fe L_2,3 edge core level shifts are also consistent with those of Fe₃O₄. We find no Fe₃O₄ layer in junctions with normal TMR. We believe this Fe₃O₄ layer is responsible for the inverse TMR.     

Giant room-temperature magnetoresistance in polycrystalline Zn(0.41)Fe(2.59)O4 with alpha-Fe2O3 grain boundaries

A tunneling-type magnetoresistance (MR) as large as 158% is observed at T = 300 K in a polycrystalline Zn0.41Fe2.59O4 sample, in which the Zn0.41Fe2.59O4 grains are separated by insulating alpha-Fe2O3 boundaries. The huge room-temperature MR is attributed to the high spin polarization of Zn(0.41)Fe(2.59)O4 grains and antiferromagnetic correlations between magnetic domains on both sides of the insulating alpha-Fe2O3 boundary. The MR exhibits strong temperature dependence below 100 K and its magnitude is enhanced to reach 1280% at 4.2 K, which may arise from the Coulomb blockade effect.     

Analysis of atmospheric corrosion products of steel and coated steel by means of scattering Mössbauer spectrometry

Wearthering steels treated with and without zinc phosphate solution were exposed to atmosphere for 15 years and rust layers produced on the steels were analysed by scattering Mössbauer spectrometry (CEMS and XMS). γ-FeOOH, fine α-FeOOH, 5Fe₂O₃·9H₂O, γ-Fe₂O₃ and Fe₃O₄ were identified to be present in the rust formed on the steel without phosphate coating. Large particles of γ-Fe₂O₃ and Fe₃O₄ formed on the uncoated steel exposed to atmosphere in a position facing north on vertical plane. The layer structure of rust was affected by the position. The thin rust layer formed on the phosphate + carylite resin coated steel was considered to consist of γ-FeOOH, fine α-FeOOH, and fine γ-Fe₂O₃.     

Hydrothermal synthesis and structural characterization of (1−x)α-Fe2O3-xSnO2 nanoparticles

Structural and morphological characteristics of (1−x)α-Fe₂O₃-xSnO₂ (x=0.0-1.0) nanoparticles obtained under hydrothermal conditions have been investigated by X-ray diffraction (XRD), transmission Mössbauer spectroscopy, scanning and transmission electron microscopy as well as energy dispersive X-ray analysis. On the basis of the Rietveld structure refinements of the XRD spectra at low tin concentrations, it was found that Sn⁴⁺ ions partially substitute for Fe³⁺ at the octahedral sites and also occupy the interstitial octahedral sites which are vacant in α-Fe₂O₃ corundum structure. A phase separation of α-Fe₂O₃ and SnO₂ was observed for x≥0.4: the α-Fe₂O₃ structure containing tin decreases simultaneously with the increase of the SnO₂ phase containing substitutional iron ions. The mean particle dimension decreases from 70 to 6 nm, as the molar fraction x increases up to x=1.0. The estimated solubility limits in the nanoparticle system (1−x)α-Fe₂O₃-xSnO₂ synthesized under hydrothermal conditions are: x≤0.2 for Sn⁴⁺ in α-Fe₂O₃ and x≥0.7 for Fe³⁺ in SnO₂.     

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.     

The properties of acicular particles of (γ-Fe2O3)x(Fe3O4)1-x

It is known that acicular particles, initially of Fe₃O₄, which have been partially oxidised, show anomalous properties e.g. in the variation of H_c with composition. It is shown that these can be explained by considering the particles to comprise an inner core of Fe₃O₄ with an outer layer of γ-Fe₂O₃. Owing to the large change in volume which occurs on oxidation, these mutually stress each other. Over a certain range of composition, the stress field interacts with the magnetization to increase H_c, and it is also responsible for H_c increasing with time after the oxidation process. A similar situation applies to partially reduced γ-Fe₂O₃.     

Synthesis and magnetic characterization of Zn0.7Ni0.3Fe2O4 nanoparticles via microwave-assisted combustion route

We report on the synthesis of Zn_0.7Ni_0.3Fe₂O₄ nanoparticles via microwave assisted combustion route by using urea as fuel. XRD and FT-IR analyses confirm the composition and structure as spinel ferrite. The crystallite size estimated from XRD (16.4 nm) and the magnetic core size (15.04 nm) estimated from VSM agree well, while a slightly smaller magnetic diameter reflects a very thin magnetically dead layer on the surface of the nanoparticles. Morphological investigation of the products was done by TEM which revealed the existence of irregular shapes such spherical, spherodial and polygon. Magnetization measurements performed on Zn_0.7Ni_0.3Fe₂O₄ nanoparticles showed that saturation was not attained at even in the high magnetic field. The sample shows superparamagnetic behavior at around the room temperature and ferromagnetic behavior below the blocking temperature which is measured as 284 K.     

Structure, band offsets and photochemistry at epitaxial α-Cr2O3/α-Fe2O3 heterojunctions

We test the hypothesis that electron-hole pair separation following light absorption enhances photochemistry at oxide/oxide heterojunctions which exhibit a type II or staggered band alignment. We have used hole-mediated photodecomposition of trimethyl acetic acid chemisorbed on surfaces of heterojunctions made from epitaxial α-Cr₂O₃ on α-Fe₂O₃(0001) to monitor the effect of UV light of wavelength 385 nm (3.2 eV) in promoting photodissociation. Absorption of photons of energies between the bandgaps of α-Cr₂O₃ (E_g = 4.8 eV) and α-Fe₂O₃ (E_g = 2.1 eV) is expected to be strong only in the α-Fe₂O₃ layer. The staggered band alignment should then promote the segregation of holes (electrons) to the α-Cr₂O₃ (α-Fe₂O₃) layer. Surprisingly, we find that the α-Cr₂O₃ surface alone promotes photodissociation of the molecule at hν = 3.2 eV, and that any effect of the staggered band alignment, if present, is masked. We propose that the inherent photoactivity of the α-Cr₂O₃(0001) surface results from the creation of bound excitons in the surface which destabilize the chemisorption bond in the molecule, resulting in photodecomposition.     

Characterization of the Calcination Products of the Precipitates Obtained from the Bio-Oxidation with Thiobacillus Ferrooxidans of Sulphuric Water Pickling Liquors

The characterization of the calcination products of the precipitates obtained from the bio-oxidation with Thiobacillus ferrooxidans of sulphuric water pickling liquors has been carried out by means of Mössbauer spectroscopy, x-ray powder diffraction, infrared spectroscopy and transmission electron microscopy. The results show that a full transformation of the precipitates into α-Fe₂O₃ is achieved at temperatures higher than 850°C. Calcination at 700°C during two hours results in the formation of α-Fe₂O₃, ζ-Fe₂O₃ and Fe₁₂O₃(SO₄)₁₅. The Mössbauer parameters of ζ-Fe₂O₃ and Fe₁₂O₃(SO₄)₁₅ at 298 and 17K are reported.