Ge_xSi_1-x_/Si应变层超晶格的分子束外延生长及其特性研究

在 Si (l00) 衬底上用分子束外延在不同的温度下生长了不同组份的GeGe_xSi_1-x_/Si 应变层超晶格.用反射式高能电子衍射、x 射线双晶衍射、卢瑟福背散射、透射电子显微镜以及Raman散射等侧试方法研究了Ge Ge_xSi_1-x_/Si超晶格的生长及其结构特性. 结果表明, 对不同合金组份的超晶格, 其最佳生长温度不同. x值小, 生长温度高; 反之, 则要求生长温度低. 对于x为0. 1-0. 6 , 在400-600℃ 的生长温度范围能够长成界面平整、晶格完好和周期均匀的GeGe_xSi_1-x_/Si应变层超晶格. 关键词：     

原位中子衍射研究两相NiTi合金的微力学相互作用和相变机理

NiTi合金的形状记忆效应与其微观结构特征密切相关,中子衍射技术可以在力学加载过程中原位观察块体NiTi合金的相变、晶间应变以及孪晶再取向等演化特征．结合两相NiTi合金宏观应力一应变曲线呈现的四种阶段性变形特征,利用原位中子衍射技术对其变形过程中的微观结构演化进行了分析．奥氏体初始体积份额约22％,在低应变硬化阶段,晶面（110）B2和（002）B19,的应变分别突然减小和增大表明出现了应力诱发马氏体相变,奥氏体体积份额迅速减小,产生了（011）II型孪晶;同时初始马氏体也开始发生再取向,随着应变量的增加,开始出现新的{20i}型马氏体孪晶,这种孪晶引起的应变卸载时不能回复．在高应变硬化阶段孪晶变形起主导作用,衍射峰半高宽变化较小;而在应变硬化饱和阶段则以滑移机制为主,大量位错的产生使衍射峰半高宽显著增加．     

Ba TiO3/SrTiO3超晶格Bragg衍射及其理论模拟

用X射线全外反射掠入射衍射和通常Bragg衍射,研究了Ba TiO³/SrTiO³(BTO/STO)超晶格的界面应变.X射线衍射动力学理论用于模拟Bragg衍射.发现与一般半导体外延膜或超晶格不同,BTO/STO超晶格的垂直和水平晶格常数的关系不完全遵守四方畸变的规律.这种偏离可能与钙钛矿型氧化物材料的结构复杂性有关.     

半导体应变超晶格结构与界面的X射线双晶衍射研究

本文应用X射线在畸变晶体中的动力学衍射理论,分析了超晶格衍射峰强度分布的规律,计算了应变超晶格中界面变化,层厚波动对双晶摇摆曲线的影响,并初步探讨了超晶格衍射峰之间的小峰消失以及衍射峰宽化的原因,研究表明,衍射峰强度分布依赖于超晶格周期中层厚、成份及应变的综合效果,界面和层厚波动将对摇摆曲线产生一定影响,而晶格弯曲是使衍射峰宽化的主要原因。     

Fe基纳米晶合金的晶化机理研究

根据用原子力显微镜对在不同温度下晶化的Fe基非晶合金薄带三维介观结构的观察,结合X射线衍射、Mssbauer谱等前人已有的实验结果并在目前已有的理论研究基础上,对Fe基非晶合金薄带在不同温度下的晶化过程进行了系统的分析、研究,提出了两种Nb-B框架介观结构、团聚相和单位体积纳米晶粒平均数等新概念,建立了Fe基纳米晶合金的晶化机理假说,提出了描述Fe基非晶合金晶化过程的介观织构模型.这个模型能够演化成二相结构模型和三相互套结构模型,还可以合理地解释现有的实验结果以及500—600℃退火中Fe基纳米晶巨磁阻 关键词： Fe基纳米晶合金 晶化机理 两种Nb-B框架介观结构 团聚相     

SmCo7纳米晶合金晶粒组织热稳定性的热力学分析与计算机模拟

推导出了单相纳米晶合金的晶界过剩体积与晶粒尺寸之间的定量关系, 建立了纳米晶合金的晶界热力学性质随温度和晶粒尺寸发生变化的确定性函数. 针对SmCo₇纳米晶合金, 通过纳米晶界热力学函数计算和分析, 研究了单相纳米晶合金的晶粒组织热稳定性. 研究表明, 当纳米晶合金的晶粒尺寸小于对应于体系中晶界自由能最大值的临界晶粒尺寸时, 纳米晶组织处于相对稳定的热力学状态; 当纳米晶粒尺寸达到和超过临界尺寸时, 纳米晶组织将发生热力学失稳, 导致不连续的快速晶粒长大. 利用纳米晶合金热力学理论与元胞自动机算法相耦合的模型对SmCo₇纳米晶合金在升温过程中的晶粒长大行为进行了计算机模拟, 模拟结果与纳米晶合金热力学模型的计算预测结果一致, 由此证实了关于纳米晶合金晶粒组织热稳定性的研究结论. 关键词： 纳米晶合金热力学 7纳米晶合金')" href="#">SmCo₇纳米晶合金 热稳定性 计算机模拟     

Nd0.5Sr0.4Pb0.1MnO3的结构和磁性

通过室温下的中子衍射和磁性测量对多晶样品Nd0.5Sr0.4Pb0.1MnO3的结构和磁性进行了实验研究.中子衍射结果表明,该样品具有正交的钙钛矿结构,空间群是Pnma,即结构发生了晶场畸变.由M-T和R-T曲线可知,居里温度TC=273 K,其特征是随着温度的增加样品经历了从铁磁金属态转变到顺磁半导态,且转变温度Tp＝225 K;用锰氧化物晶场和双交换作用的竞争解释了其温度Tp以下的金属特性.     

Nd0.5Sr0.4Pb0.1MnO3的结构和磁性

通过室温下的中子衍射和磁性测量对多晶样品Nd_0.5Sr_0.4Pb_{0 .1}MnO₃ 的结构和磁性进行了实验研究.中子衍射结果表明，该样品具有正交的钙钛矿结构，空间群 是Pnma，即结构发生了晶场畸变.由M-T和R-T曲线可知，居里温度T_C=273 K ，其特征是随着温度的增加样品经历了从铁磁金属态转变到顺磁半导态，且转变温度T _p＝225 K；用锰氧化物晶场和双交换作用的竞争解 关键词： 结构 磁性 中子衍射 晶场畸变 p')" href="#">转变温度T_p 双交换作用     

低温固相反应法制备的NiFe2O4纳米颗粒的结构与磁性

采用低温固相反应法制备了晶粒尺寸在8—47nm之间的NiFe₂O₄纳米颗粒系列样品，用X射线衍射仪(XRD)、高分辨中子粉末衍射谱仪、振动样品磁强计和超导量子干涉仪等对样品的晶体结构、宏观磁性和纳米颗粒的表面各向异性进行了分析研究.XRD和中子衍射测量结果显示纳米颗粒的晶格常数略高于块体材料，样品的氧参量表明纳米颗粒的晶格畸变程度没有块体材料严重.相对块体材料，纳米颗粒具有较小的磁化强度、较大的矫顽力和各向异性能密度.纳米颗粒从多畴转变为单畴的临界尺寸约为40nm，超顺磁性临界尺寸约为16nm.     

Y-Ba-Cu-O化合物的晶体结构畸变对超导性能的影响

本文研究了不同处理条件(烧结后不同冷却速度和在不同气氛中时效)产生的晶格畸变对Y-Ba-Cu-O化合物超导性能的影响。结果发现,随烧结后的冷速增加,正交层状钙铁矿相的三对X射线主衍射峰的强度逐渐发生反转现象,伴随超导性能的改变。同时,该化合物超导体与水蒸汽、CO等极性分子间存在着强烈的交互作用,使得正交相的衍射峰的强度发生相似变化,并可导致样品在液氮温区失超。这说明正交相的畸变与Y-Ba-Cu-O化合物的超导性能有着密切的关系。并由实验结果的分析和计算揭示了二者的定量关系。同时,用极化理论和晶体场模型就畸变对超导性能的影响作了定性的解释。     

Magnetic octupole order in : A polarized neutron diffraction study

Recently, in phase IV of Ce_xLa_1-xB₆, weak but distinct superlattice reflections from the order parameter of phase IV have been detected by our unpolarized neutron scattering experiment [K. Kuwahara, K. Iwasa, M. Kohgi, N. Aso, M. Sera, F. Iga, J. Phys. Soc. Japan 76 (2007) 093702]. The scattering vector dependence of the intensity of superlattice reflections is quite unusual; the intensity is stronger for high scattering vectors. This result strongly indicates that the order parameter of phase IV is the magnetic octupole. However, the possibility that the observed superlattice reflections are due to lattice distortions could not be completely ruled out only on the basis of the unpolarized neutron scattering experiment. To confirm that the superlattice reflections are magnetic, therefore, we have performed a single crystal polarized neutron diffraction experiment on Ce_0.7La_0.3B₆. The obtained result has clearly shown that the time reversal symmetry is broken by the order parameter of phase IV. This is further evidence for the magnetic octupole order in Ce_xLa_1-xB₆.     

Austenitic structure formation in an Fe-32% Ni alloy during slow heating in the critical temperature range

Electron diffraction is used to show (for the first time) that the reverse α → γ transformation in an Fe-32% Ni during slow heating develops via the formation of an intermediate paramagnetic 9R phase. Coarse extended lamellae form according to a shear mechanism in the central part of the temperature range of the reverse transformation, which is called the critical range (here, the physical properties of the alloy change anomalously). The extended lamellae consist of 9R-phase lamellae with γ-phase interlayers. A high density of periodic stacking faults in the structure of the 9R phase and a high density of chaotic stacking faults in the complex 9R + γ phase determine the nature of phase transformation-induced hardening.     

中子衍射法研究单晶镍基高温合金热机械疲劳引起的应力和晶格错配

采用中子衍射法对热机械疲劳后的单晶镍基高温合金样品内部中心点进行了实验测量,数据处理采用了双相叠加峰和单峰分析两种方法,计算得到了样品材料的宏观等效应力、应力偏量、γ相和γ′相的等效应力和晶格错配度等.实验结果表明,两种分析方法得到的宏观等效应力基本一致.在热机械疲劳循环100周出现最大宏观等效应力和应力偏量,此时位错等微缺陷达到饱和,偏离中心点处γ′相应力减小显著;在热机械疲劳开始阶段负错配度明显减小,随循环周次增多基体塑性应变累积又使负错配度以每次81×10^-6的速度逐渐线形增大. 关键词： 中子衍射 单晶高温合金 等效应力 应力偏量     

The evolution of γ-Mg17Al12 intermetallic compound during accumulative back extrusion and subsequent ageing treatment

Accumulative back extrusion (ABE) processing, as a novel severe plastic deformation (SPD) method, has been recently justified to be capable of modifying the microstructural characteristics of alloys. In line to its ongoing researches, the present work has been planned to study the evolution of γ-Mg₁₇Al₁₂ intermetallic phase during ABE and subsequent ageing treatment in a high Al-bearing Mg–Al–Zn alloy. The behaviour of γ intermetallic has been systematically examined as following points of view: (i) strain–temperature-dependent morphology changes, (ii) strain-induced dissolution, and (iii) re-ageing behaviour as a function of time and temperature. Aiming to analyse the morphology of eutectic γ compound with respect to the strain and temperature, 2D projections of effective diameter, shape factor and globularity have been made in strain/temperature graphs. The processing conditions (strain and temperature) corresponding to the desired and undesired morphologies are introduced and microstructurally explained through underlying plasticity mechanisms, i.e., ‘necking-thinning-particle separation’ and ‘brittle fragmentation.’ The former mechanism is suggested to be in relation with partial strain-induced dissolution of eutectic γ phase, leading to generation of a supersaturated solid solution. This has resulted to the observation of ‘off-stoichiometry’ phenomena in Mg₁₇Al₁₂ phase and has been justified through dislocation-assisted deformation mechanism at elevated temperature. Surprisingly, a unique re-ageing behaviour has been found for the obtained solid solutions, where a modified kinetics and morphology of γ phase precipitation were characterized. The altered precipitation behaviour is attributed to the specific defect structure achieved by SPD acting as fast diffusion channel for Al solutes.     

Investigation of phase transition of γ-alumina to α-alumina via mechanical milling method

In this research, the results obtained from studying the phase transition of γ-alumina (γ-Al₂O₃) to α-alumina (α-Al₂O₃) during intense mechanical activation in high-energy ball milling are presented. The powder samples were characterized by scanning electron microscope (SEM), X-ray diffraction (XRD), thermogravimetric and Differential thermal analyses (TG-DTA). With respect to the results achieved from above analyses, the transition of γ → α-alumina through δ- and θ-phases, can be initiated. Also, it was found that the pure γ-alumina phase showed a great stability during high-energy ball milling and there was no transformation to any other phase after a long milling time (30 h). On the other hand, γ-alumina containing a small amount of the α-alumina seed, showed a gradual phase transition from γ-alumina to α-alumina in milling. The phase transition mechanism during milling is nucleation and growth, which is promoted by the α-alumina seed.     

Synthesis,phase stability and oxide ion conductivity of Ce(IV)–Cd(II) double substituted bismuth vanadate

Bi₄V₂O_11-δ has been doped with Ce and Cd to study double substitution. The system with various dopant concentrations (0.07 ≤ x ≤ 0.30) was prepared by the standard solid-state reaction method. The correlation between the polymorphism and oxide ion performance was well investigated as a function of temperature and composition with the help of thermal analysis, X-ray diffraction (XRD) and AC impedance spectroscopy. From XRD results it is seen that the high oxide ion conducting tetragonal γ-phase is stabilized for x = 0.17. For the compositions x ≤ 0.10, monoclinic α-phase is retained at room temperature with clear evidence for two successive phase transitions α ? β and β ? γ. For x = 0.13, β ? γ phase transition is seen. However, the existence of order–disorder, γ' ? γ transition was confirmed for x = 0.17. It is seen that the highest low-temperature ionic conductivity at 320 °C is 3.19 × 10^?4 S cm^?1 which was observed for x = 0.17.     

Correlation between phase structure and electrical conduction in BISNVOX system for intermediate temperature solid oxide fuel cells (IT-SOFC)

Samples of Sn⁴⁺-substituted bismuth vanadate, formulated as Bi₄Sn _x V_{2? x} O_{11?( x /2)? δ} in the composition range 0.07 ≤ x ≤ 0.30, were prepared by standard solid-state reactions. Sample characterization and the principal phase transitions (α ? β, β ? γ and γ′ ? γ) were investigated by FT-IR spectroscopy, X-ray powder diffraction, differential thermal analysis (DTA) and AC impedance spectroscopy. For composition x = 0.07, the α ? β and β ? γ phase transitions were observed at temperatures of 451 and 536°C, respectively. DTA thermograms and Arrhenius plots of conductivities revealed the γ′ ? γ phase transition at 411 and 423°C for x = 0.20 and 0.30, respectively. AC impedance plots showed that conductivity is mainly due to the grain contribution, which is evident in the enhanced short-range diffusion of oxide ion vacancy in the grains with increasing temperature. The highest ionic conductivity (5.03 × 10^?5 S cm^?1 at 300°C) was observed for the x = 0.17 solid solution with less pronounced thermal hysteresis.     

The structure of the γ phase of palladium deuteride

Single crystal neutron diffraction measurements of superlattice reflections in Pd/D have been used to determine the structure of a new ordered phase (γPd/D) existing below 50 K. This phase is stabilised by nearest and next nearest neighbour repulsive interactions.     

水热体系TeO2-K3PO4-H2O中一个新化合物——K2Te4O9·3H2O的合成与结晶

作者用水热法对TeO₂-K₃PO₄-H₂O体系作了初步的合成与结晶尝试。在给定的条件和组成范围内除了能形成TeO₂晶体外,还能生成一种点阵参数为a=b=10.734?,c=21.041?,α=β=90°,γ=120°的三方晶系的化合物γ,其分子式为K₂Te₄O₉·3H₂O。结晶区的产物主要取决于原料的k=TeO₂/K₃PO₄(克分子比:当k≤1.9时,仅生成γ晶体;k≥2.22时,单独生成TeO₂晶体;而当1.92晶体出现,本文还给出了γ晶相的DTA曲线和X射线粉末衍射谱线的相对强度与相应面间距的详细数据。 关键词：