PARALLEL AUXILIARY SPACE AMG FOR H（curl） PROBLEMS

In this paper we review a number of auxiliary space based preconditioners for the second order definite and semi-definite Maxwell problems discretized with the lowest order Nedelec finite elements. We discuss the parallel implementation of the most promising of these methods, the ones derived from the recent Hiptmair-Xu （HX） auxiliary space decomposition [Hiptmair and Xu, SIAM J. Numer. Anal., 45 （2007）, pp. 2483-2509]. An extensive set of numerical experiments demonstrate the scalability of our implementation on large-scale H（curl） problems.     

Live retention database for identification of compounds in capillary gas chromatographic analysis --Principle and structure

A live retention database for compound identification in isothermal and any step temperature programmed capillary gas chromatography has been developed. The database utilizes the Kovats retention indices of compounds on a given stationary phase and the retention time of n-alkanes measured at isothermal conditions on the column to be used, together with the programming parameters. Identification is performed by search operation that compares the calculated results with the retention values of unknown peaks. Cross-reference of the search results of different operating conditions is performed automatically by the database in order to increase the reliability of the identification. The error of the database conversion is ≤± 0.5 index unit, or ≤± 1% on retention time. This paper describes the principle and the structure of the database in detail. The experimental results for different calsses of compounds tested at divers operating conditions will be presented in Part Ⅱ.     

低泵浦能量类氖锗等离子体软X射线激光实验

提出并采用具有一定时间间隔的双束脉冲加热锗薄膜靶方法，在泵浦激光能量１００Ｊ，靶长１０ｍｍ的实验条件下，观察到波长１９．６１ｎｍ和２３．６３ｎｍ两条类氖锗３ｓ－３ｐ激光跃迁线。１９．６１ｎｍ（Ｊ＝０－１）的激光跃迁线发射强度较２３．６３ｎｍ（Ｊ＝２－１）激光线的强度大，其发散角较后者小。     

一台小型强流脉冲离子束加速器

 介绍了一台小型强流脉冲离子束加速器的结构组成,采用箍缩反射型离子二极管,可以稳定工作的峰值电压为200kV,得到了峰值为1.5kA、脉宽约20ns的离子束流,平均离子流密度110A/cm²。     

Blow up problem for Landau-Lifshitz equations in two dimensions

In 1986, Zhou and Guo in [1] proved the global existence of weak solution for generalized Landau-Lifshitz equations without Gilbert term in multi-dimensions. They consider thehomogeneous boundary problemwith the initial value conditionfor the system of ferromagnetic chain with several variableswhere j(x, t, Z) is a given 3-dimensional vector funC-non in x e R", t E R+, Z e R', W(x)is a given 3-dimensional initial value function on fi, fi is a bounded domain in n-dimensionalEuclidean space…     

光系统ⅡChl分子能量传递超快光谱动力学

利用ICCD飞秒扫描成象和飞秒时间分辨光谱装置实验研究了高等植物捕光天线LHCⅡ三聚体和PSⅡ颗粒复合物的超快光谱动力学,经过吸收光谱和发射光谱分析,确定在LHCⅡ三聚体中至少存在7种Chl分子光谱特性,分别是Chlb_653/656^658.7、Chla_662.0^665.2、Chla/b_670/671^677.1、Chla_675.0^677.1、Chla_680/681^682.9、Chla_685.0^689.1和Chla_695.0^695.6.采用光强1013光子/cm²/脉冲激励浓度为30μg/mL的捕光天线LHCⅡ三聚体,在650nm到705nm谱段逐点探测分析处理,产生了2组短寿命组分210fs、520fs和5.2ps、36.7ps及2个长寿命组分1.8ns、2ns.最快的3个寿命210fs、520fs和5.2ps反映了三聚体Chlb分子向Chla分子的激发能传递过程;寿命36.7ps反映了Chla分子向相邻单体Chla分子的激发能传递过程;最长的2个寿命1.8ns和2ns是在三聚体中Chla分子通过中间体Chla分子辐射荧光,分别跃迁回基态的过程.获得的6个寿命组分有把激发能传递时间与Chla/b分子发射光谱相结合的特点.经拟合处理解析PSⅡ颗粒复合物光谱,得到3个组分谱,其峰值分别为686.8nm、692.2nm和694.9nm,与LHCⅡ比较分析,说明天然构型的PSⅡ有很强的吸收光能和有效传递光能的本领.     

氧碘化学激光器UR-90腔光束质量研究

 概括了光束质量的表示方法, 由衍射极限倍数的定义出发, 提出重点在于选取光斑直径, 而且可把光斑测量归结到电子测试仪对剪切电平的测量上。给出了电子测试仪的测试原理, 由所测光斑直径计算了氧碘化学激光器U R290腔的光束质量指标—衍射极限倍数, 达到了1.2～1.6倍衍射极限, 最后进行了误差讨论。     

主脉冲参数和入射条件变化对等离子体状态的影响

用一维非平衡辐射流体力学程序，计算和分析了主脉冲激光斜入射与预脉冲垂直入射耦合作用锗靶介质的等离子体状态和激光增益区。研究表明，主脉冲以４０°斜入射与其垂直入射相比，在相同靶面功率密度下，电子、离子温度、等离子体烧蚀深度下降约１０％。在相同的靶面总能量下，４０°斜入射电子温度下降约１５％～２０％。采用主激光斜入射时间延迟技术，这种下降差别还会更小，能量吸收效率会更高，激光增益区更大。     

Scaling Behaviour of Diffusion Limited Aggregation with Linear Seed

We present a computer model of diffusion limited aggregation with linear seed. The clusters with varying linear seed lengths are simulated, and their pattern structure, fractal dimension and multifractal spectrum are obtained. The simulation results show that the linear seed length has little effect on the pattern structure of the aggregation clusters if its length is comparatively shorter. With its increasing, the linear seed length has stronger effects on the pattern structure, while the dimension D f decreases. When the linear seed length is larger, the corresponding pattern structure is cross alike. The larger the linear seed length is, the more obvious the cross-like structure with more particles clustering at the two ends of the linear seed and along the vertical direction to the centre of the linear seed. Furthermore, the multifractal spectra curve becomes lower and the range of singularity narrower. The longer the length of a linear seed is, the less irregular and nonuniform the pattern becomes.     

Sol-Gel Method for Preparation of LiLaNiO/γ-Al_2O_3 Catalyst over Monoliths used in POM Reaction

Partial oxidation of methane (POM) has several advantages over the traditional industrial method of steam reforming, such as much higher space velocity, reduced capital and operation cost and optimized the ratio of the products (H2/CO). Many investigators are interested in the POM reaction over monolith now1-3. Monolith is a kind of ceramic-like metal oxide material. It has relative high surface to volume ratio compared to commercial pellets, low pressure drop during the reaction process2,…