第十四届国际材料强度大会简介

2006年6月5—9日，第十四届国际材料强度大会（14th International Conferenceon the Strength of Materials，IC-SMA14）在西安古都新世界大酒店举行，会议正式代表322人（其中境外代表200多人），这是该系列国际材料强度大会第一次在中国举办．大会由中国国家自然科学基金委员会、国家教育部、中国材料研究学会、西安交通大学、中国科学院沈阳金属研究所和西安市科技局等单位共同支持．大会主席为J．L．Martin教授，会议组织委员会主席由西安交通大学的孙军教授与中国科学院金属研究所的李守新研究员共同担任．

Yb∶Y_3Al_5O_(12)/Y_3Al_5O_(12)复合晶体的制作和光谱性能

采用热键合技术,制作中运用不同的工艺参量制作出12片Yb∶Y3Al5O12/Y3Al5O12(Yb∶YAG/YAG)复合晶体。利用偏光显微镜对其键合界面进行了观察,研究了样品的透射光谱,从而确定出复合晶体合适的制作工艺。通过透射光谱的形状和透射率来表征复合晶体键合界面的质量。研究表明Yb∶YAG/YAG复合晶体键合质量较好,可实现一体化。

不同处理方式采伐剩余物的分解及其对森林更新的影响

采伐迹地上运走大径级的原木所剩下的枝桠物质是生态系统养分能量的来源；是动力，植物和微生物物栖息地。在本世纪五十年代就有人（A. A. Loman）对择伐和皆伐迹地上的枝桠进行了研究，用以比较它们树皮存留率的差异，但详细深入的研究是在八十年代以后，以R. L. Edmonds, C. E. Pertson为代表研究不同层次，不同径级研究枝桠的分解速率，我国在此领域的研究尚属空白。本文以长白山阔叶红松林带的四个树种：红松，白桦，落叶松，色木为对象探讨了它们枝桠的生物量，分解速率，分解过程中的养分动态以及枝桠堆对更新和火灾的影响。采伐后0-14后间，迹地上枝桠干重为31.96-9.60T/ha，通过对7个年代采伐迹地上枝桠堆面积估算后得知，枝桠堆平均占地为11.53%，以1CM直径累计值对应的枝桠堆的高度（Y：CM）为因变量，分解时间（X, yr）为自变量，则枝桠堆高度随时间变化的过程可以描述为：Y = 1.288 - 0.000889 X~2 r = -0.9896。本文以密度（Y: g/CM~3）随分解年令（X: yr）的变化来表示分解速率。四十年代样品用排水法求出来的密度与用园柱法求出的密度有如下相关关系：Y排 = 0.0129 +2.316 Y园，r = 0.94 Y表示密度（g/CM~3）。我们用单项指数模型描述分解速率：落叶松：Y = 0.4701 * exp (-0.01783 X) r = -0.927 色木: Y = 0.6742 * exp (-0.07824 X) r = -0.988 红松：Y = 0.5349 * exp (-0.03421 X) r = -0.927 桦树：Y = 0.5316 * exp (-0.1139 X) r = -0.992 红松树皮的分解模型近似于直线：Y = 0.5258 - 0.01133 X r = -0.984 落叶松，红松，色木，桦树的分解常数分别为：0.01783, 0.0.41, 0.0782, 0.1139。依此预测分解原密度的95%所需要的时间分别为：168年，87.6年，38.3年，26年。可以看出这四个树种分解从难到易的顺序为：落叶松 > 红松 > 色木 > 桦树。对枝桠密度的差民显著性检验可以说明：红松样品层次对分解的影响显著而径级对分解的影响仅在下层显著。随着分解的进行，样品的重量损失，我们也探讨了密度的降低与失重百分率之间的关系。桦树样品下层失重比上层快，说明淋溶作用对桦树样品失重的贡献不大。温湿度是影响分解的最主要的生态因子。枝桠堆上下层的湿度差异特别明显。分解时间越长，径级对含水量的影响越显著。水分含量（Y：%）随年代（X: yr）变化的趋势为：Y = 36.18 - 0.004337 X~2 (4-7cm径级）Y = 33.64 - 0.01097 X~2 (1-4cm径级） 温，湿度影响土壤动物及微生物种群分布及数量，进而影响到枝桠的分解速率，分解过程中元素动态变化是：C基本上恒定，全N含量趋于增高。径级对红松N的累积有影响。下层4-6cm径极累积最快，其次是上层4-6cm。层次的影响仅限于红松，除72年以外上层 > 下层。其它元素如P, Mg++， Ca++总的趋势是随分解过程而增加。土壤中的C元素含量受立地条件的影响，但是枝桠堆下面土壤C值高于对照。枝桠堆对森林更新和火灾均有影响。枝桠是林火的燃料，枝桠堆面积占采伐迹地的11.53%，这样减少更新面积。

Preparation and transport properties of a bulk icosahedral quasicrystalline Ti45Zr35Ni17Cu3 alloy

A bulk alloy which consists of the single icosahedral quasicrystalline phase (I-phase) in Ti45Zr35Ni17CU3 alloy has been fabricated by mechanical alloying and subsequent pulse discharge sintering technique. Crystallographic structure analyses show that the bulk alloy is an I-phase. The transport properties of the bulk alloy are examined, and the results show that the room-temperature thermal conductivity is 5.347 W K-(1) m(-1), and the electrical conductivity decreases with increasing the temperature from 300 to 450K. The Seebeck coefficient is negative at the temperature range from 300 to 360K, and changes to positive from 370 to 450K. Hall effect measurements indicate the bulk I-phase alloy has a high carrier concentration. The specific heat capacity increases when the temperature increases from 280 to 324 K.

Study on the instability of organic field-effect transistors based on fluorinated copper phthalocyanine

The effects of positive and negative gate-bias stress on organic field-effect transistors (OFET) based on tantalum (Ta)/tantalum pentoxide (Ta2O5)/fluorinated copper phthalocyanine (F16CuPc) structure are investigated as a function of stress time and stress temperature. It is shown that gate-bias stress induces a parallel threshold voltage shift (DeltaV(T)) of OFETs without changes of field-effect mobility mu(EF) and sub-threshold slope (DeltaS). The DeltaV(T) is observed to be logarithmically dependent on time at high gate-bias appropriate to OFET operation. More importantly, the shift is directional, namely, be large shift under positive stress and almost do not move under negative stress. The threshold voltage shift is temperature dependent with activation energy of 0.51 eV We concluded that threshold voltage shift of the OFET with F16CuPc as active layer is due to charge trapping in the insulator in which trapped carriers have redistribution.

青藏高原高寒湿地生态系统CO_2通量

依据涡度相关系统连续观测的2005年CO_2通量数据,对青藏高原东北隅的高寒湿地生态系统源/汇功能及其部分环境影响因素进行了分析。结果表明,高寒湿地生态系统为明显的碳源,在植物生长季（5-9月份）吸收230.16 gCO_2•m~(-2),非生长季（1-4月份及10-12月份）释放546.18 gCO_2•m~(-2),其中净排放最高在5月份,为181.49 gCO_2•m~(-2),净吸收最高在8月份,为189.69 g CO_2•m~(-2),年释放量为316.02 gCO_2•m~(-2)。在平均日变化中,最大吸收值出现在7月份12：00,为（0.45±0.0012）mgCO_2•m~(-2)•s~(-1),最大排放速率出现在8月份0：00,为（0.22±0.0090）mgCO_2•m~(-2)•s~(-1)。生长季中6-9月份表现为明显的单峰型日变化,非生长季的变化幅度较小。净生态系统交换量（NEE）和生态系统总初级生产力（GPP）与气温、空气水气饱和亏和地表反射率等环境因素呈现相似的相关性,与地上生物量和群落叶面积指数则为线性负相关,生态系统呼吸（Res）则与上述因子的相关性呈现相反的趋势。

ADI方法求解Navier-Stokes方程的一个改进格式

ADI方法常被用来计算不可压缩Navier-Stokes方程。在处理涡度方程的非线性项和涡度在壁面上的条件时,通常采用滞后的方法对涡度方程和流函数方程分别求解。然而,非线性项的滞后破坏了ADI方法的完全二阶精度;涡度方程和流函数方程分别求解减弱了两个方程的耦合性;涡度壁面条件的滞后则破坏了方法的完全隐式。本文在应用ADI方法求解涡度方程和流函数方程时应用了一种交替线性化的技术,对涡度方程和流函数方程耦合求解,内点和边界点上的涡度和流函数值同时求出。因此,ADI方法保持了完全的二阶精度,避免了上面所提到的问题。作者应用这一方法计算了雷诺数R_θ等于1,10,100,500,1000时的二维方腔流动(空间步长h=1/20)。计算结果表明:这一方法保持了通常ADI方法的优点,可以应用大的时间步长。最后补充计算了雷诺数R_θ=2000的二维方腔流动。

Mixed-mode fracture mechanisms near the fatigue threshold of aisi-316 stainless-steel

Near threshold, mixed mode (I and II), fatigue crack growth occurs mainly by two mechanisms, coplanar (or shear) mode and branch (or tensile) mode. For a constant ratio of ΔK_I/ΔK_II the shear mode growth shows a self-arrest character and it would only start again when ΔK_I and ΔK_II are increased. Both shear crack growth and the early stages of tensile crack growth, are of a crystallographic nature; the fatigue crack proceeds along slip planes or grain boundaries. The appearance of the fracture surfaces suggest that the mechanism of crack extension is by developing slip band microcracks which join up to form a macrocrack. This process is thought to be assisted by the nature of the plastic deformation within the reversed plastic zone where high back stresses are set up by dislocation pile-ups against grain boundaries. The interaction of the crack tip stress field with that of the dislocation pile-ups leads to the formation of slip band microcracks and subsequent crack extension. The change from shear mode to tensile mode growth probably occurs when the maximum tensile stress and the microcrack density in the maximum tensile plane direction attain critical values.

Sequence context analysis of 8.2 million single nucleotide polymorphisms in the human genome

We analyzed n-mers (n=3-8) in the local environment of 8,249,446 human SNPs and compared their distribution with that in the genome reference sequences. The results revealed that the short sequences, which contained at least one CpG dinucleotide, occurred

草鱼、中华鳖IL-2活性影响因素的研究

结果显示 :当年草鱼种和中华鳖脾细胞培养上清液中能检测出IL 2活性 ,而且 1龄以上草鱼、中华鳖的IL 2活性高于当年孵化的草鱼和中华鳖。草鱼、中华鳖脾细胞在 2 5℃培养温度条件下 ,其上清液中IL 2活性最高 ,35℃次之 ,1 5℃最低。因此 ,草鱼、中华鳖IL 2活性在一定范围内是随着年龄增加而增强和依赖温度的。通过小鼠胸腺细胞增殖和对小鼠L92 9细胞杀伤率的实验表明 37℃比 2 5℃检测温度下所测的IL 2活性高 ,而中华鳖胸腺细胞增殖实验却显示 2 5℃检测温度下IL 2活性高于 37℃

Luminescence study of (11(2)over-bar0) GaN film grown by metalorganic chemical-vapor deposition

Investigations on photoluminescence properties of (11 (2) over bar0) GaN grown on (1 (1) over bar 02) Al2O3 substrate by metalorganic chemical-vapor deposition are reported. Several emission lines not reported before are observed at low temperature. The sharp peak at 3.359 eV is attributed to the exciton bound to the neutral acceptor. Another peak at 3.310 eV represents a free-to-bound, probably a free electron-to-acceptor, transition. The 3.241 and 3.170 eV lines are interpreted as phonon replica lines of the 3.310 eV line. The phonon energy is 70 meV, consistent with the energy of transverse optical E-1 phonon. The optical properties of the lines are analyzed. (C) 2003 American Institute of Physics.

Hydrothermal synthesis and crystal structure of a novel compound: [Ni(phen)(3)](2)[(SiMo10V2O40)-O-IV((VO)-O-IV)2]center dot 2H(2)O

A novel compound [Ni(phen)(3)](2)[(SiMo10V1/2O40)-O-V((VO)-O-IV)(2)] . 2H(2)O has been hydrothermally synthesized and structurally characterized by single-crystal X-ray diffraction. The compound crystallizes in the triclinic, system, space group P-1, a = 12.378(4) Angstrom, b = 14.148(5) Angstrom, c = 14.316(2) Angstrom, alpha = 105.91(2)degrees, beta = 95.31(2)degrees, gamma = 96.89(3)degrees, V = 2373.0(12) Angstrom(3), Z = 1, (lambdaMo(Kalpha)) = 0.71073 Angstrom, R1 (wR2) = 0.0869(0.2174). Data were collected on a Siemens P4 four-circle diffractometer at 293 K in the range of 1.51 < theta < 22.50degrees using the omega-scan technique. Empirical absorption correction (psi scan) was applied. The structure was solved by the direct method and refined by the Full-matrix least-squares on F-2 using the SHELXL-97 software. X-ray crystallographic study showed that the title compound contained a bi-capped alpha-Kegin-type [(SiMo10V2O40)-O-IV((VO)-O-IV)(2)](4-) polyoxoanion.