混合氧化物掺杂电致变色

本文论述采用混合氧化物掺杂的新方法,对电致变色层和离子导电层分别掺入氧化物和金属,使电致变色器件响应速度、增大着色透过率变化等方面的特性得到很大改善.最后给出实验结果.     

固体电解质Li9-nxMn+xN2Cl3(M=Na、Mg、Al)的合成及表征

高温固相反应合成了固体电解质Li_(9-nx)M~(n )_xN_2Cl_3(M=Na、Mg、Al)。利用粉末 X射线衍射测定样品结构。测定了离子电导率 ,分解电压和电子电导。得出掺杂可以提高快离子导体材料 Li_9N_2Cl_3的电导率。并讨论了掺杂阳离子的半径和价态与替代离子的关系和影响。使用 x=0.05mol的二价镁离子替代 Li_9N_2Cl_3中的 Li＋离子可以很大程度的提高其电导率。     

(Ba,Ca)(Co,Fe)O3-δ系列混合导电型透氧膜的研究

采用改进的Ｐｅｃｈｉｎｉ法合成了（Ｂａ,Ｃａ）（Ｃｏ,Ｆｅ）Ｏ３－δ系列材料,对其结构,透氧量及透氧稳定性进行了考察,结果表明,材料具有较高的透氧量和透氧稳定性,其中Ｂａ０．９５Ｃａ０．０５Ｄｏ０．８Ｆｅ０．２Ｏ３－δ在９５０℃透氧量高达１．４ｍｌ／（ｃｍ＾２．ｍｉｎ）,８５０℃稳定操作１６０ｈ以上,将其应用于膜反应器,对无催化剂的甲烷氧化偶联反应作了尝试,结果表明,对甲烷氧化偶联反应具有较高的选择,但甲烷转化率较低。     

考虑温度效应的覆冰导线动力学建模及舞动特征研究

针对以往研究忽略了温度效应对覆冰导线舞动特性的影响,本文推导了考虑温度效应影响的覆冰导线舞动控制方程。基于悬链法、热应力理论推导了覆冰导线的偏微分舞动方程,接着通过Galerkin法将该偏微分方程转化为常微分方程。建立气动载荷模型,将气动力引入到舞动方程中,随后采用多尺度求得了覆冰导线的位移响应,最后进行了参数分析、算例分析。结果表明:温度对覆冰导线面内、面外的频率影响显著,且对覆冰导线舞动的幅值也有一定的影响。可见针对覆冰导线舞动特征的影响研究,有必要考虑温度效应的影响,本文的研究成果有利于理论建模的完善,也能给予实际工程一定的参考。     

Optical microstrip patch antennas design and analysis

This paper has presented transparent conductor oxide materials (TCOMs) based microstrip patch antennas with glass substrate and copper ground plane, which have been deeply analyzed in the visible spectrum region in comparison with the practical patch antenna model of indium tin oxide patch with glass substrate and different TCOMs based ground plane. As well as the study have investigated the effect of transparent oxide materials on patch antenna design instead of perfect conductor materials such as copper that has low cost and weight. The tradeoff between optical transparency and electrical conductivity will be evaluated for a range of visible regions. Microstrip transmission line feed method is used to predict the skin effects on a patch antenna and their impact on antenna efficiency, resonance frequency and optical transmission are also described. This study have discussed assessment of these tradeoffs and effect of TCOMs parameters on antenna design.     

Defects,phase transitions and dynamical disorder in superionic protonic conductors H3OUO2PO4 · 3H2O and CsHSO4

Specific properties of the hydrogen bond and protons appear to be responsible for the formation of the quasi-liquid state of conducting ions and the resulting superionic behaviour. This state is reached by successive phase transitions involving the mobile species and their interactions with a more or less rigid framework. H₃OUO₂PO₄ · 3H₂O (HUP) and CsHSO₄ can be considered as models of wet and dry superionic conduction, respectively. Interactions between static effects and dynamical disorder as well as the coupling between sublattices are discussed in relation to results obtained by calorimetry, impedance spectroscopy (up to 10 GHz), vibrational spectroscopy and quasi-elastic neutron scattering.     

Temperature dependence of Bi2O3 structural parameters close to the α–δ phase transition

This article presents the results of in situ X-ray powder diffraction, Raman spectroscopy, and electrical impedance spectroscopy of the α-phase of Bi₂O₃, at 0.1 MPa in the temperature range below and above the α–δ-phase transition. This work demonstrated subtle nonlinear temperature variations of the cell parameters, of the hard-mode Raman shift, and of the activation energy of electrical conductivity in the temperature range about 100–120°C below the α–δ phase transition temperature T _Tr ≈ 725°C in Bi₂O₃. At T < 600°C, the linear variation of the inverse dielectric susceptibility (χ ^?1) correlates well with the hard mode frequency shift Δ(ω ²) of Raman A_1g mode as Δ(χ ^?1)/Δ(ω ²) ≈ 5.5 × 10^?7 cm². A structural model describing the mechanism of O^2? anion distribution and electric dipole disordering in the vicinity of T _Tr is discussed.     

Influence of anionic substitution on phase transitions in Cu6PS5I1− x Cl x mixed crystals

Cu₆PS₅I_{1? ?} ? _x Cl _x mixed crystals were grown using chemical vapour transport. Isoabsorption studies of optical absorption edge and optical polarization measurements were performed in the temperature range 77–320?K. The influence of anionic I?→?Cl substitution on the phase transitions in Cu₆PS₅I_{1? ?} ? _x Cl _x mixed crystals is studied. Compositional dependence of the phase-transition temperatures is obtained and the x,T-diagram for Cu₆PS₅I_{1? ?} ? _x Cl _x mixed crystals is constructed.     

BaSnF4 fast ion conductor: Variations versus the method of preparation and anomalous temperature variation of the quadrupole splitting

A new method of preparation of high performance fluoride ion conductor, BaSnF₄, by water leaching of newly discovered barium tin(II) chloride fluorides, has been designed, and the materials have been studied and compared to the solid prepared by the usual dry method. The unit-cell parameters and crystallite dimensions were found to vary with the method of preparation. In addition, the crystallite dimensions were found to be highly anisotropic for the samples obtained by the wet method. The Mössbauer spectrum is made of a large tin(II) quadrupole doublet, and a broad tin(IV) oxide peak due to surface oxidation. The tin(II) spectrum is in agreement with covalently bonded tin(II) having a strongly stereoactive lone pair. An unusually high dependence of the quadrupole splitting at low temperatures was observed (5.8 times larger than for α-SnF₂).     

Development of cube textured Ni–5 at.%W alloy substrates for coated conductor application using a melting process

Biaxially textured Ni–5 at.%W substrates have been prepared by cold rolling, followed by three different annealing routes. In this paper, the processes of melting Ni and W metals, flat rolling, various annealing methods are described in detail. The Ni–5 at.%W tapes annealed under either high vacuum or flowing Ar (7% H₂) gas were characterized by X-ray pole figures, ODF, EBSD as well as AFM analysis. The texture analysis indicated that as fabricated tapes have a sharp cube texture formed after annealing at a wide temperature range of 800–1100 °C. The high quality of cube orientation on tapes was obtained after a two-step annealing (TSA), where the percentage of the cube texture component was as high as 93.5% within a misorientation angle smaller than 8° from EBSD analysis. Furthermore, it was also observed that the number of twin boundaries in this tape decreased with respect to that of tapes annealed both in vacuum and one-step gas annealing. From AFM on 1 μm² areas, it was concluded that the roughness (RMS) on the tape surface reached 0.98 nm.