The AgxCu1−xInS2 solid solutions with 0≤x≤1

The phase equilibriums in the AgInS2–CuInS2 system were investigated by means of X-ray diffraction and differential thermal analysis and the AgInS2 and CuInS2 ternary compounds and the AgxCu1–xInS2 solid solutions were grown by two-zone horizontal method with the following directed crystallization of melt. The T–x phase diagram of this system was constructed and the formation of solid solutions in the complete range of compositions was discovered. The composition dependencies of microhardness, transmission spectra in the range of the fundamental absorption, infrared transmission spectra in the range from 150 to 400 cm-1 for the AgxCu1–xInS2 solid solutions were investigated. It was discovered that the composition dependence of microhardness is expressed by smooth curve having maximum for x=0.2. The composition dependencies of band gap have been analytically expressed at 77 and 293 K for the Ec and Ec direction of polarization and have non-linear behaviour. From the studies of the infrared transmission spectra the frequencies of optical phonons were determined and it was discovered that their composition dependence shows single mode behaviour.     

Oxidation behavior of Mo≤5Si3C≤1 and its composites

The oxidation behavior of Mo₅Si₃C₁ and its composites was studied in air over the temperature range of 500°C–1600°C. Experiments revealed poor oxidation resistance of monolithic Mo₅Si₃C₁ at high temperature. The oxidation was quite rapid at 1200°C and above, resulting in complete oxidation of specimens in a short time. The addition of 2.0 wt% boron was found to produce a Mo₅Si₃C₁ composite with three other phases of MoB, MoSi₂, and SiC, and showed remarkable improvement in oxidation resistance. The mechanism for the improvement was attributed to the viscous sintering of the scale to close the pores formed during the initial oxidation period. Oxidation tests were also conducted on SiC-Mo₅Si₃C₁ composite at 800°C, 1300°C and 1600°C for more than 100 hours. The oxidation resistance of the composite was found to be very good. The results demonstrate that, though oxidation resistance of monolithic Mo₅Si₃C₁ is far insufficient for high-temperature applications, boron-modification and/or composites with SiC are viable methods to improve oxidation resistance to a practically acceptable level.     

Phase diagram of the CrxVSe2 system (0 ≤ x ≤ 1.0)

The phase diagram of the pseudo-binary CrVSe₂ (i.e. Cr_xVSe₂) system was determined by means of X-ray and DTA measurements, in the composition range 0≤x≤1.0. As the results, the following 6 phases have been confirmed to be existent in the temperature range 300≤T≤1100 : CdI₂,M₅X₈,M₃X₄,α,NiAs and Cr. Among them, M₅X₈,M₃X₄ and α phases undergo a phase transition to the CdI₂- or NiAs-type structures at high temperatures. The α phase (0.825≤x≤0.875 at 500°C) is a new phase firstly confirmed by this study.     

Specific Heat of LaMnO3 + δ at 50 K ≤ T ≤ 160 K

We have developed a shell model, which includes the long-range coulomb, van der Waals interaction, and the short-range Hafemeister–Flygare repulsive interaction operative up to second neighbor atom to study the cohesive and thermal properties of LaMnO_{3 + δ}. The results on cohesive energy obtained by us are in good agreement with that of calculated value by DeSouza et. al. (R. A. DeSouza, M. S. Islam, and E. I. Tiffee, J. Mater. Chem. 9, 1621 (1999)). In addition, we have also calculated molecular force constant (f), compressibility (β), restrahlen frequency (ν_o), Debye temperature (Θ_D), and the low temperature specific heat at 50 K ≤ T ≤ 160 K. Our results on Debye temperature and specific heat for the temperature range 50 K ≤ T ≤ 160 K are closer to the recently measured data with an automated quasi-adiabatic pulse technique.     

Diffusion of mercury into for HgxCd(1−x)Te 0≤x≤0.03

Experiments carried out to fabricate Hg_xCd_(1-x)Te by diffusing mercury into CdTe slices from the vapour, resulted in obtaining slices with a maximum value of x=0.004. Measurements on the diffusion of mercury into such slices, where 0≤x≤0.03, under saturated vapour pressure conditions, resulted in two component profiles, each profile giving two values of D. These results were similar to ones obtained earlier, indicating that the diffusion was rate-limiting. In addition, the diffusivities were found to be independent of x. This revised version was published online in July 2006 with corrections to the Cover Date.     

LiGdxMn2-xO4(0≤x≤0.1)材料的结构与电化学性能

采用高温固相法合成掺杂Gd3+的锰酸锂LiGdxMn2+O4(x=0、0.01、0.05、0.1)锂离子电池正极材料并研究了其结构与电化学特性.XRD分析表明,随着Gd3+含量的增加,材料的晶格参数、晶胞体积、Mn-Mn、Mn-O键距、Mn3+/Mn4+比值均下降,材料结构稳定性得到改善.当x≥0.05时第二相Gd2O...     

Conduction in nanostructured La1?x Sr x FeO3 (0 ≤ x ≤ 1)

We investigated electrical properties of nanostructured La_1?x Sr _x FeO₃ (0 ?? x ?? 1) from 300 K?C400 K. The nanostructured La_1?x Sr _x FeO₃ (0 ?? x ?? 1) was synthesized by citrate gel method requiring no pH control. X-ray diffraction pattern showed that single phase LaFeO₃ with an orthorhombic structure was formed. The structure changed into rhombohedral for x = 0.5 and it became cubic for x = 1.0. For x ?? 0.5, our material showed non-linear current-voltage characteristics and for x > 0.5 it showed linear current-voltage characteristics. Poole Frenkel type conduction mechanism was found to be operative in LaFeO₃ from 300 K?C400 K. The experimental values of field-lowering coefficient were by 2.56?C6.41 times higher than the predicted value and were attributed to the presence of localized fields. The increase in conductance with Sr content was due to formation of Fe⁴⁺ ions in addition to Fe³⁺ with the increase in Sr content. Impedance spectroscopy and ac conductivity analysis of La_1?x Sr _x FeO₃ (0 ?? x ?? 1) was also carried out in the temperature range from 300 K?C400 K and frequency was varied from 20 Hz - 2 MHz. The ac conduction followed the correlated barrier hopping model in La_0.9Sr_0.1FeO₃.     

Specific Heat of LaMnO3 + δ at 50 K ≤ T ≤ 160 K

We have developed a shell model, which includes the long-range coulomb, van der Waals interaction, and the short-range Hafemeister–Flygare repulsive interaction operative up to second neighbor atom to study the cohesive and thermal properties of LaMnO_{3 +} . The results on cohesive energy obtained by us are in good agreement with that of calculated value by DeSouza et. al. (R. A. DeSouza, M. S. Islam, and E. I. Tiffee, J. Mater. Chem. 9, 1621 (1999)). In addition, we have also calculated molecular force constant (f), compressibility (), restrahlen frequency (_o), Debye temperature (_D), and the low temperature specific heat at 50 K T 160 K. Our results on Debye temperature and specific heat for the temperature range 50 K T 160 K are closer to the recently measured data with an automated quasi-adiabatic pulse technique.     

Hydrothermal Synthesis and Transport Properties of FeS1-xTex (0 ≤ x ≤ 0.15) Single Crystals

Journal of Superconductivity and Novel Magnetism - In this work, a series of FeS1-xTex (0 ≤ x ≤ 0.15) single crystals were successfully synthesized by a hydrothermal method for the...     

Comment on the magnetic properties of the system Sr2−xCaxFeMoO6, 0≤x≤2

The structural and magnetic properties of the n-type-metallic double-perovskite system Sr_2−xCa_xFeMoO₆ are reported. At 5 K, the saturation magnetization remains M_s(5 K)=3.5 μ_B/formula unit compared to a theoretical spin-only moment of 4.0 μ_B/formula unit for a perfectly ordered compound. From the shape of the M–H hysteresis loops below T_c, it is suggested that ferromagnetic long-range ordered domains are coupled antiferromagnetically across antiphase boundaries; random disorder within domains may be small. An unprecedented dependence of the paramagnetic susceptibility on the applied magnetic field is reported and attributed to an overlapping Fe³⁺/Fe²⁺ and Mo⁶⁺/Mo⁵⁺ redox couple, first suggested by Sleight and Weiher [Sleight AW, Weiher JF. J. Phys Chem Solids 1972; 33: 679.], which results in localized S=5/2 spins on the iron atoms coexisting with itinerant minority-spin electrons in a narrow π* band.     

钙钛矿La0.7-xNdxSr0.3MnO3(0.1≤x≤0.6)的结构及磁性研究

采用溶胶-凝胶法制备了钙钛矿L20.7-xNdxSr0.3MnO3(0.1≤x≤0.6)系列样品,经过X射线衍射仪(XRD)、扫描电镜(SEM)、振动样品磁强计(VSM)等表征,结果表明,当Nd的掺杂量x≤0.4时,样品保持单相,样品L20.7-xNdxSr0.3MnO3均属于正交晶系,x＞0.4时,样品由和L20.7-xNdxSr0.3MnO3和Nd2O3两相组成.样品的颗粒形貌呈现比较规则的立方体.颗粒的尺寸不太均匀,边长一般在1～3μm之间.随着Nd掺杂量的增加,样品的居里温度逐渐降低,居里温度附近的最大磁熵变逐渐增大.     

Statistical model for molten Fe1−yCryNx (0·4≤y≤0·9)

Abstract

Results of previous statistical thermodynamic analysis appeared to imply that N atoms in molten Fe_1?yCr_y (0·05<y<0·2) are trapped in octahedral voids (O-sites) surrounded by one Cr atom and five Fe atoms. However, previous work did not include development of a statistical model for molten Fe_1?yCr_yN_x-with higher Cr content. In the present work, available equilibrium nitrogen pressure–temperature–composition relationships for molten Fe_1?yCr_yN_x were analysed in the composition range 0·4≤y≤0·9. The results of the present analysis appeared to suggest that in this composition range O-sites surrounded by four Cr atoms and two Fe atoms provide the trapping sites for N atoms.

MST/721     

Thermoelectric Properties of TlIn1 – x Yb x Te2 (0.01 ≤ x ≤ 0.09) Crystals

The thermoelectric properties of TlIn_{1 – x} Yb _x Te₂ (0.01 x 0.09) crystals are studied. The results indicate that the crystals possess high thermoelectric figures of merit in the range 500–700 K.     

Preparation and Structure of Ga2 – x Sc x O3 (0.42 ≤ x ≤ 0.52)

The structure of a scandium gallium oxide single crystal grown by the Czochralski process from a charge of composition Ga_1.5Sc_0.5O₃ is determined by x-ray diffraction. The structure is shown to be a superstructure to -Ga₂O₃. The superstructure parameters are found to vary both along the axis of the crystal and radially, which is due to variations in Ga : Sc ratio. A structural model of the Ga_1.5Sc_0.5O₃ crystal is proposed.     

钙钛矿型Gd1-xDyxMnO3(O≤x≤1)的水热合成及磁性表征

通过环境友好的水热法制备了钙钛矿型稀土锰酸盐Gd1-xDyxMn℃3(0≤x≤1),该系列化合物具有正交结构(属于pbnm空间群).在合成反应中,Mn(OH)2在强碱体系下被空气中O2氧化生成包含Mn3+的反应前驱物;锰酸盐的晶体生长、反应温度和碱度对其有明显的影响.磁性表征结果显示Dy3+对Gd3+的取代引起了化合物低温磁有序的竞争.     

Magnetic Properties and Metamagnetic Transition in SmCo1−x Fe x AsO (0≤x≤0.2)

Polycrystalline SmCo_1?x Fe _x AsO (x=0, 0.05, 0.1, 0.2) materials with single phase have been synthesized by solid-state reaction. According to the X-ray diffraction patterns, the a-lattice parameter shrinks, but the c-lattice parameter expends with the increased amount of Fe doping. Complicated magnetisms consist of antiferromagnetic, ferromagnetic, and paramagnetic have been observed between 5 K and 300 K in the present system. Magnetic measurement shows that with increasing Fe content, antiferromagnetic order of SmCoAsO is suppressed and ferromagnetic order is enhanced. Below their antiferromagnetic transition temperature, metamagnetic transition can be detected in samples with x<0.2, and the transition field decreases with increasing Fe content. When Fe content reaches 0.2, no metamagnetic transition is observed down to 5 K. A canting of the spins plays a crucial role in metamagnetic behavior of the present system.     

The penetration depth of HgBa2CuO4+δ with 0.07 ≤ δ ≤ 0.35

The magnetic penetration depth (T) of three HgBa₂CuO₄₊ samples with 0.16 < 0.27 has been determined from the reversible magnetization. The obtained follows a BCS-like correlation of 1/² 1–(T/T_c)² over whole measured temperature range in an underdoped sample with T_c 90 K, but deviates significantly from similar fits in an overdoped sample with the same T_c and an optimum doped sample, whose 1/² 's depends on T nearly linearly below T_c/2. This asymmetry between the underdoped and overdoped samples suggests that the T-dependence of 1/² is affected by doping in a complicated way.     

z≤16的齿轮测量中的一个问题

《计量技术》辑编部: 根据机械工业部部标《渐开线圆柱齿轮精度》(JB179—83)要求,确定渐开线齿形测量部位,一般用两种方法;第一、按共轭齿轮啮合时的工作圆计算;第二、在相配齿轮不清楚时,按与标准齿条啮合时的工作圆计算。在按第二种方法计算齿廓起测点展开弧长b_1(或展开角φ_1,下同)时,一般都认为:齿数z≤16齿的齿轮,基圆半径r_b大于齿轮与标准齿条啮合时的工作圆半径R(即过齿条齿顶线与啮合线的交点T的圆,如图1所示),这时不需计     

低温燃烧法合成Ce1-xNdxO2-x/2（0≤x≤0．6）纳米粉体

采用低温燃烧合成法，在柠檬酸-硝酸盐体系中合成出Ce1-xNdxO2-x/2（0≤x≤0．6）固溶体纳米粉体。X射线衍射（XRD）结果表明，Nd^3＋取代Ce^4＋进入晶格内部，形成具有单相立方萤石结构的固溶体，其晶格常数随Nd^3＋掺杂浓度的增大而线性增加，晶粒尺寸在15-24nm之间。透射电镜（TEM）结果表明，粉体颗粒尺寸在20-40nm之间，分散性较好，具有较高的烧结活性。拉曼光谱（Raman Spectrum）结果表明，F2g宽化峰的出现与掺杂后固溶体中产生的氧空位有关，并且随着掺杂浓度的增加，氧空位数量也再增加。