945 resultados para Ti-Mo alloys


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The interface states of [NiFe/Mo](30) and [Fe/Mo](30) multilayers have been investigated by x-ray small angle reflection and diffuse scattering. Significant interface roughness correlation was observed in both ultrathin [NiFe/Mo](30) and [Fe/Mo](30) multilayers. An uncorrelated roughness of about 27-3.1 Angstrom was revealed in the [NiPe/Mo](30) multilayers, which is explained as originating from a transition layer between the NiFe and the Mo layers. By the technique of diffuse scattering, it is clearly indicated that the interfacial roughness of NiFe/Mo is much smaller than that of Fe/Mo although the lattice mismatch is the same in both multilayers.

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We have measured photoluminescence of ZnSxTe1-x alloys (x > 0.7) at 300 K and under hydrostatic pressure up to 7 GPa. The spectra contain only a broad emission band under excitation of the 406.7 nm line. Its pressure coefficients are 47, 62 and 45 meV/GPa for x = 0.98, 0.92 and 0.79 samples, which are about 26%, 7% and 38% smaller than that of the band gap in the corresponding alloys. The Stokes shifts between emission and absorption of the bands were calculated by fitting the pressure dependence of the emission intensity, being 0.29, 0.48 and 0.13 eV for the three samples, respectively. The small pressure coefficient and large Stokes shift indicate that the emission band observed in our samples may correspond to the Te isoelectronic center in the ZnSxTe1-x alloy.

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Raman scattering studies were reported of In1-x-yGaxAlyAs/InP lattice matched quaternary alloys. The quaternary alloys a.ere grown on (100) oriented InP substrates by MBE method. The composition and intensity dependence of optical phonon mode frequencies show that the quaternary alloys exhibit three-mode behavior, i.e. InAs-like, GaAs-like and AlAs-like modes. Polarization analysis of the Raman spectra shows that the LO phonon modes are Raman active in the depolarized configuration and Raman inactive in the polarized configuration. TO phonon modes were also observed due to disorder effects, resulting in the asymmetrical shapes of the Raman peaks of the optical phonons.

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High amounts of acid compounds in bio-oil not only lead to the deleterious properties such as corrosiveness and high acidity, but also set up many obstacles to its wide applications. By hydrotreating the bio-oil under mild conditions, some carboxylic acid compounds could be converted to alcohols which would esterify with the unconverted acids in the bio-oil to produce esters. The properties of the bio-oil could be improved by this method. In the paper, the raw bio-oil was produced by vacuum pyrolysis of pine sawdust. The optimal production conditions were investigated. A series of nickel-based catalysts were prepared. Their catalytic activities were evaluated by upgrading of model compound (glacial acetic acid). Results showed that the reduced Mo-10Ni/gamma-Al2O3 catalyst had the highest activity with the acetic acid conversion of 33.2%. Upgrading of the raw bio-oil was investigated over reduced Mo-10Ni/gamma-Al2O3 catalyst. After the upgrading process, the pH value of the bio-oil increased from 2.16 to 2.84. The water content increased from 46.2 wt.% to 58.99 wt.%. The H element content in the bio-oil increased from 6.61 wt.% to 6.93 wt.%. The dynamic viscosity decreased a little. The results of GC-MS spectrometry analysis showed that the ester compounds in the upgraded bio-oil increased by 3 times. it is possible to improve the properties of bio-oil by hydrotreating and esterifying carboxyl group compounds in the bio-oil.

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Low pressure metalorganic chemical vapour deposition (LP-MOCVD) growth and characteristics of InAssb on (100) Gasb substrates are investigated. Mirror-like surfaces with a minimum lattice mismatch are obtained. The samples are studied by photoluminescence spectra, and the output is 3.17 mu m in wavelength. The surface of InAssb epilayer shows that its morphological feature is dependent on buffer layer. With an InAs buffer layer used, the best surface is obtained. The InAssb film shows to be of n-type conduction with an electron concentration of 8.52 x 10(16) cm(-3).

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本论文首先研究了Ni、Zr分别对Ti-V-Cr固溶体储氢合金中Cr和Ti部分取代的影响,得到了性能良好的Ti0.17Zr0.08V0.35Cr0.10Ni030基质合金。在此基础上进一步研究了入甄、B、Fe、Co、Al元素的添加或取代对基质合金的结构及电化学性能的影响。采用XRD、ICP、SEM一EDX、XPS、EIS、线性极化和阳极极化等表征手段对Ti一V-Cr固溶体储氢合金的结构及电化学性能进行分析和表征,主要结果如下:①Ti一V-Cr合金自身在碱性电解液中几乎无电化学活性。当用Ni部分取代Cr后,合金中出现具有电化学活性的第二相,其电化学性能得到有效地改善和提高。②Ti0.25-xZr_xV0.35Cr0.1Ni0.3(x=0.05-0.15)合金主要是由bcc相和c14Laves相组成。随Zr含量从0.05增加到0.08,合金电极的放电容量和倍率放电能力增加;当x继续从0.08增加到0.15时,其变化较小。合金电极的电荷转移电阻随x增加而降低,当x在0.08到0.15之间变化时,电荷转移电阻变化也比较小。表明电荷转移电阻的大小与合金的电化学性能密切相关。③经过50次充、放电循环后,Tio.17zr"sV时scrol0Ni03。合金电极在303K和313K的放电容量能保持在90%以上;在70℃时的放电容量仍能达到275mA扮g。根据不同温度时的交换电流密度,计算了Ti。,17Zr008V时SCr川0Ni030合金电极表面电化学反应的表观活化能,其值约为50kJ/mol。④通过Nln、B、Fe、C。、AI对Tio.17zroosvo35Crol0Nio3。合金基质的添加与取代的研究,得到了具有高容量的储氢合金。其中Tio.17Zr008Vo35Cro.10Ni020Mnol。合金室温最高放电容量达到390n1A扮g;在253一343K的温度范围内,Tiol7Zr08V035Cr0JONioz5Mnoos合金具有高的放电容量,其容量在167一298mA树g之间变化,但是这些合金的稳定性有待进一步的提高。⑤合金充、放电过程中,晶格的扭曲和膨胀、Zr和V的溶解使得合金结构发生变化;合金的严重粉化及表面致密氧化膜的形成,是导致Ti一V-Cr合金电化学性能的衰减的主要原因。