(Ni0.8Zn0.2Fe2O4)epoxy-PZT双层膜中的磁电效应

讨论了Ni0.8Zn0.2Fe2O4(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(αE)的最大值变化范围为25.6 mV Am-2≤αE≤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.     

纳米MFe2O4（M=Ni,Zn）氧化物表面的光电子能谱

采用草酸共沉淀法制备了纳米MFe2O4（M=Ni,Zn）立方尖晶石粉体,分别用XRD、XPS等手段对所合成样品的相结构、表面元素状态进行了表征。Fe2p、O1s的XPS分析表明,氧化物表面存在Fe2＋及吸附态氧物种,氧空位的存在是形成反式尖晶石结构所致。     

Fe掺杂La0．8Sr0．2Co1-xFexO3磁性的研究

利用溶胶-凝胶法制备了一系列的La0.8Sr0.2Co1-xFexO3样品.通过研究在不同外加磁场下磁化强度和温度变化的关系发现,在较高的外场下La0.8Sr0.2Co1-xFexO3样品的磁性反转现象没有被观察到;在低场下La0.8Sr0.2Co1-xFexO3系统磁性反转现象被实现.这说明Fe的掺杂引起了La0.8Sr0.2Co1-xFexO3样品中铁磁和反铁磁之间的竞争,导致了La0.8Sr0.2Co1-xFexO3样品磁性反转;同时外加磁场的强弱影响了La0.8Sr0.2Co1-xFexO3系统磁性反转现象的发生,外加磁场增大使得在La0.8Sr0.2Co1-xFexO3样品中Co离子的自旋平行趋势更强,在铁磁和反铁磁之间的竞争中铁磁耦合占主导优势,因此在较高的外场下磁性反转现象没有被观察到.     

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     

基于LiCo0.8M0.2O2 (M=Ni,Zr)薄膜的全固态薄膜锂电池

用射频磁控溅射结合传统退火的方法制备LiCo0.8M0.2O2 (M=Ni,Zr)阴极薄膜．X射线衍射、拉曼光谱、扫描电子显微镜等手段表征了不同掺杂的LiCo0.8M0.2O2薄膜．结果显示,700℃退火的LiCo0.8M0．2O2薄膜具有类似α-NaFeO2的层状结构．通过对不同掺杂锂钴氧阴极的全固态薄膜锂电池Li／LiPON／LiCo0.8M0.2O2的电化学性能研究表明,电化学活性元素Ni的掺杂使全固态电池具有更大的放电容量(56μAh／cm2μm),而非电化学活性元素Zr的掺杂使全固态电池具有更好的循环稳定性．     

H2O2氧化法制备Fe3O4纳米颗粒及与共沉淀法制备该样品的比较

在近中性条件下,利用H2O2氧化Fe(OH)2胶体成功制备了Fe3O4纳米颗粒.分别利用透射电镜(TEM),x射线衍射仪(XRD),振动样品磁强计(VSM)和超导量子干涉仪(SQUID)对样品的形貌,结构,宏观磁性进行了表征和测量.TEM图像表明样品为球形颗粒,直径大小约18nm,且分布较均匀.XRD结果表明样品为立方尖晶石结构.穆斯堡尔谱测量表明样品室温下对应两套六线谱,样品的晶体结构存在缺陷,内磁场略小于块体Fe3O4的值.宏观磁测量表明样品的饱和磁化强度可达67×10-3A·m2/g,在20 K出现了Verwey转变.选择该法制备的Fe3O4纳米颗粒与共沉淀法得到的样品作了磁性比较.宏观磁测量表明共沉淀法制备的样品在外磁场为1T时仍未饱和,磁化强度仅为46×10-3A·m2/g,在178K出现了超顺磁转变温度,且在测量温度范围内没有发现Verwey转变.     

MSM结构Mg0.2Zn0.8O可见盲光电探测器

采用射频磁控溅射,通过传统的紫外曝光和湿法腐蚀的方法,制备了不同电极间距的金属-半导体-金属(MSM)结构Mg0.2Zn0.8O可见盲光电探测器.研究了器件的暗电流和响应度随电极间距的变化关系,当施加的电压没有达到贯穿电压的时候,暗电流和响应度均随着电极间距的增加而减小,并对其具体的机制进行了研究.     

La0.8Sr0.2Co1-xFexO3材料局域结构的研究

采用溶胶-凝胶法制备了La0.8Sr0.2Co1-xFexO3样品,并测量了各样品的X射线衍射谱（XRD）和X射线吸收精细结构（XAFS）谱。XRD分析研究发现Fe的掺杂引起了La0.8Sr0.2CoO3材料相分离;在前期对X射线吸收精细结构谱近边分析的基础上,进一步分析扩展边X射线吸收精细结构谱,表明在La0.8Sr...     

Co/Ni多层膜垂直磁各向异性的研究

采用直流磁控溅射法在玻璃基片上制备了Pt底层的Co/Ni多层膜样品, 对影响样品垂直磁各向异性的各因素进行了调制, 通过样品的反常霍尔效应系统的研究了Co/Ni多层膜的垂直磁各向异性. 结果表明, 多层膜中各层的厚度及周期数对样品的反常霍尔效应和磁性有重要的影响. 通过对多层膜各个参数的调制优化, 最终获得了具有良好的垂直磁各向异性的Co/Ni多层膜最佳样品Pt(2.0)/Co(0.2)/Ni(0.4)/Co(0.2)/Pt(2.0), 经计算, 该样品的各向异性常数K_eff 达到了3.6×10⁵ J/m³, 说明样品具备良好的垂直磁各向异性. 最佳样品磁性层厚度仅为0.8 nm, 样品总厚度在5 nm以内, 可更为深入的研究其与元件的集成性.     

钙钛矿型锰氧化物(La_(0.8)Eu_(0.2))_(4/3)Sr_(5/3)Mn_2O_7的磁性和电性研究

采用传统固相反应法制备钙钛矿型锰氧化物(La0.8Eu0.2)4/3Sr5/3Mn2O7多晶样品,X-射线衍射分析表明,样品(La0.8Eu0.2)4/3Sr5/3Mn2O7结构呈现良好的单相.通过磁化强度随温度的变化曲线(M-T)、不同温度下磁化强度随磁场的变化曲线(M-H)和电子自旋共振谱发现:在300 K以下,随着温度的降低,样品先后经历了二维短程铁磁有序转变(T2D C≈282K)、三维长程铁磁有序转变(T3D C≈259K)、奈尔转变(T N≈208K)和电荷有序转变(T CO≈35K);样品(La0.8Eu0.2)4/3Sr5/3Mn2O7在T N以下,主要处于反铁磁态;在T3D C达到370 K时,样品处于铁磁-顺磁共存态,在370 K以上时样品进入顺磁态.此外,分析电阻率随温度的变化曲线(ρ-T)得到:样品在金属-绝缘转变温度(T P≈80K)附近出现最大磁电阻值,其位置远离T3D C,表现出非本征磁电阻现象,其磁电阻值约为61%.在T CO以下,电阻率出现明显增长,这是由于温度下降使原本在高温部分巡游的e g电子开始自发局域化增强所致.通过对(La0.8Eu0.2)4/3Sr5/3Mn2O7的ρ-T曲线拟合,发现样品在高温部分的导电方式基本遵循小极化子的导电方式.     

Magnetic Behaviour of Nano-Particles of Ni0.8Cu0.2Fe2O4

Nano-particles of Ni_0.8Cu_0.2Fe₂O₄ have been synthesized by the co-precipitation method. Langevin function fitting of the superparamagnetic M–N curve at 290 K provides a log-normal distribution with median diameter of 30 Å and standard deviation of 0.4. Outside a core of ordered spins, moments in the surface layer are disordered. Magnetization evolves over a long period of time t going linearly with log t. Magnetic anisotropy which was estimated by fitting the M–log t curve shows many fold increase over that of bulk particle sample. Major contribution to this enhancement comes form the disordered surface spins.     

Effects of excessive Zn2+ ions on intrinsic magnetic and structural properties of Ni0.2Zn0.6Cu0.2Fe2O4 powder prepared by chemical coprecipitation method

Zn(OH)₂ is a kind of amphoteric compound. Therefore, for chemical coprecipitation method, the precipitation of Zn²⁺ ions may be incomplete if using NaOH as precipitator. In this study, single-phase powder specimens with a nominal composition Ni_0.2Zn_0.6Cu_0.2Fe₂O₄ were prepared with chemical coprecipitation method, and the effects of excessive Zn²⁺ content (x, x = 3%, 5%, 7%, 9%) in working solution on intrinsic magnetic and structural properties were studied by vibrating sample magnetometer and X-ray diffractometer, respectively. It was found that the magnetization when H_m = 398 kA/m (5000 Oe) reached a maximum when x = 5%, and then decreased with the increase of x, which was attributed to the effect of different amount of Zn²⁺ in A sites on the A–B and B–B exchange interaction. Moreover, it was found that the lattice parameter was affected by the Zn²⁺ and Fe³⁺ ions due to their different ion radius to a certain extent.     

On the origin of the ferromagnetism in Zn0.8Mn0.2O having a higher Curie temperature than Zn0.8Co0.2O

Zn_0.8Co_0.2O and Zn_0.8Mn_0.2O films were deposited on substrates by a sol–gel technique. X-ray diffraction, field-emission scanning electron microscopy, photoluminescence, and ferromagnetism measurements were used to characterize these dilute magnetic semiconductors. It is shown that the ferromagnetic properties might be related to the formation of acceptor-like defects in the Zn_0.8Co_0.2O and Zn_0.8Mn_0.2O films. It is found that ferromagnetic Zn_0.8Mn_0.2O has a higher Curie temperature than Zn_0.8Co_0.2O. In addition, the higher ratio of grain-boundary area to grain volume of Zn_0.8Mn_0.2O than Zn_0.8Co_0.2O indicates that grain boundaries and related acceptors are the intrinsic origin for ferromagnetism.     

Structure and oxygen stoichiometry of SrCo0.8Fe0.2O3−δ and Ba0.5Sr0.5Co0.8Fe0.2O3−δ

High temperature X-ray diffraction (HT-XRD), temperature programmed desorption (TPD), thermogravimetric analysis–differential thermal analysis (TGA/DTA) and neutron diffraction were combined to determine the structure and oxygen stoichiometry of SrCo_0.8Fe_0.2O_3−δ (SCF) and Ba_0.5Sr_0.5Co_0.8Fe_0.2O_3−δ (BSCF) up to 1273 K in the pO₂ range of 1 to 10^− 5 atm. Formation of the vacancy-ordered brownmillerite phase, SrCo_0.8Fe_0.2O_2.5, was observed as a region of zero oxygen release in the TPD measurements and confirmed by HT-XRD and TGA/DTA. No ordering was observed in the BSCF system by any of the techniques utilized in this work. The oxygen vacancy concentration of BSCF was found to be considerably higher than that of SCF and always higher than that of the ordered brownmillerite phase of SCF, δ = 0.5. The combination of a high vacancy concentration and absence of ordering leads to higher oxygen permeation fluxes through BSCF membranes in comparison to SCF.     

Oxygen reduction at sol–gel derived La0.8Sr0.2Co0.8Fe0.2O3 cathodes

The perovskite material, La_0.8Sr_0.2Co_0.8Fe_0.2O₃ (LSCF), substituted by Sr and Fe at the A and B sites, was prepared using the sol–gel (SG) method, followed by heating at 900 °C for 4 h. The X-ray powder diffraction pattern for the SG derived LSCF material showed good agreement with the literature data. Scanning electron microscopy showed that the LSCF structure is highly porous, facilitating gas transfer and maximizing the number of active sites for the oxygen reduction reaction (ORR) at the cathode of a solid oxide fuel cell. Transmission electron microscopy (TEM) was employed to determine the SG–LSCF particle size and distribution. The kinetics of the ORR were investigated at SG–LSCF, deposited by screen-printing on a samarium-doped ceria (SDC) electrolyte, using electrochemical impedance spectroscopy and cyclic voltammetry at temperatures ranging from 400 to 700 °C. The results showed that the SG–LSCF cathode is stable and exhibits a high exchange current density (and low charge transfer resistance), yielding an apparent activation energy for the ORR of ca. 120 kJ/mol. It was also found that the SG–LSCF on SDC cathode was approximately one order of magnitude more active than standard manganite-based composite cathodes, deposited on yttria stabilized zirconia, studied under otherwise identical operating conditions.     

Oxygen permeability of CaTi0.8Fe0.2O3-δ

The oxygen permeation through a dense ceramic membrane with the composition CaTi_0.8Fe_0.2O_3-δ has been measured as a function of the oxygen partial pressure gradient across the membrane at high temperatures (1000, 1050 °C). The permeation current dependence on the oxygen pressure gradient indicates that bulk diffusion controls the oxygen transport rate in the membrane under moderate oxygen pressure gradients, while the surface exchange limits the oxygen permeation at high oxygen pressure gradients. An oxygen concentration drop appears at the membrane-gas boundary.