B-(*())(B)over-bar(()*()) intermediate states contribution to Gamma(4S, 5S) -> eta(b) + gamma radiative decay

In this work, we investigate the rescattering effects in the radiative decay Gamma(5S) -> eta(b) + gamma , which were suggested to be crucially important for understanding the anomalous largeness of the branching ratios B(Gamma(5S) -> Gamma(1S) + pi pi) and B(Gamma(5S) -> Gamma(1S) + eta). Our calculations show that the rescattering effects may enhance Gamma(Gamma(10860) -> eta(b) +gamma) by four orders, but the tetraquark structure does not. Recently the BABAR and CLEO collaborations have measured the mass of eta(b) and the branching ratios B(Gamma(2S) -> eta(b) +gamma), B(Gamma(3S) -> eta(b) +gamma). We hope that very soon, Gamma(10860) -> eta(b) + gamma) will be measured and it would be an ideal opportunity for testing whether the rescattering or the tetraquark structure is responsible for the anomaly of B(Gamma(5S) -> Gamma(nS) pi(+) pi(-))(n = 1, 2, 3)), i. e., the future measurements on the radiative decays of Gamma(5S) might be a touchstone of the two mechanisms.

gamma cross section in p plus p collisions at root s=200 GeV

We report on a measurement of the gamma(1S + 2S + 3S) -> e(+)e(-) cross section at midrapidity in p + p collisions at root s = 200 GeV. We find the cross section to be 114 +/- 38(stat + fit)(-24)(+23)(syst) pb. Perturbative QCD calculations at next-to-leading order in the color evaporation model are in agreement with our measurement, while calculations in the color singlet model underestimate it by 2 sigma. Our result is consistent with the trend seen in world data as a function of the center-of-mass energy of the collision and extends the availability of gamma data to RHIC energies. The dielectron continuum in the invariant-mass range near the gamma is also studied to obtain a combined yield of e(+)e(-) pairs from the sum of the Drell-Yan process and b-(b) over bar production.

Electron impact excitation rate coefficients of N II ion

This paper calculates the electron impact excitation rate coefficients from the ground term 2s(2)2p(2) P-3 to the excited terms of the 2s(2)2p(2), 2s2p(3), 2s(2)2p3s, 2s(2)2p3p, and 2s(2)2p3d configurations of N II. In the calculations, rnulticonfiguration Dirac-Fork wave functions have been applied to describe the target-ion states and relativistic distorted-wave calculation has been performed to generate fine-structure collision strengths. The collision strengths are then averaged over a Maxwellian distribution of electron velocities in order to generate the effective collision strengths. The calculated rate coefficients are compared with available experimental and theoretical data, and some good agreements are found for the outer shell electron excitations. But for the inner shell electron excitations there are still some differences between the present calculations and available experiments.

Differential and Integral Cross Sections for Electron Impact Excitation of Lithium

The differential and integral cross sections for electron impact excitation of lithium from the ground state 1s(2)2s to excited states 1s(2)2p, 1s(2)3l (l = s,p,d) and 1s(2)4l (l = s,p,d,f) at incident energies ranging from 5 eV to 25 eV are calculated by using a full relativistic distorted wave method. The target state wavefunctions are calculated by using the Grasp92 code. The continuum orbitals are computed in the distorted-wave approximation, in which the direct and exchange potentials among all the electrons are included. A part of the cross sections are compared with the available experimental data and with the previous theoretical values. It is found that, for the integral cross sections, the present calculations are in good agreement with the time-independent distorted wave method calculation, for differential cross sections, our results agree with the experimental data very well.

缺中子核素133Sm、133Pr和93Pd的衰变

本硕士沦文籍助兰州重离子加速器国家实验室分离扇聚焦回旋加速器（SFC）提供的重离子束通过全融合蒸发反应产生远离口稳定线的缺中子核素，并用本课题组发展和建立的氦喷嘴快速带传输系统以及多重符合测量装置分离、测量核素来研究其衰变性质。在实验准备期间，曾采用~(252)Cf源进行了氦喷嘴（I－I eje咧央速带传输系统效率的测定。给出了PbI_2，PbCl_2，NaCl三种无机欲添加剂的传输效率，以及传输效率随目标核质量变化的初步结果。而后完成了以下两项物理实验：~(113)Sm的（EC＋β~+）衰变纲图和133Pr的同核异能态的研究：用SFC引出的~(40)Ca~(12+)束流轰击96%Ru的浓缩同位素靶，采用氦喷嘴带传输系统和x-γ与γ-γ符合测量方法，首次建议了~(133)Sm的简单的（EC＋β~+）衰变纲图并测得了其β衰变半衰期。~(133)Sm是目前发表过（EC＋β~+）衰变纲图的最轻的钐（Sm的缺中子核。由于Ru靶中含有~(98-102)Ru的成分，同时产生了~(133)Pr，并首次测定了~(133)Pr 11／2~－同核异能态的寿命为（l.1±0.2）s。为Pr奇A核11／2~-同核异能态的数据作了重要的补充，汇编成Pr奇A核的11／2一同核异能态和与之相关的3／2~＋，5／2~+和7／2~+能级的系统性数据。用单粒子模型理论拟合从中提取了~(131,133,135,137)Pr的11／2~-同核异能态的约化跃迁概率的实验值，并与Weisskopf近似估计进行了比较。2.~(93)Pd的β缓发质子衰变：通过~(58)Ni（~(40)Ca，3n2p）反应合成β缓发质了先驱核~(93)Pd，采用氦喷嘴带传输系统加p-γ符合观测到了它的β缓发质子衰李，测得其半衰期为1.3±0.2s。采用统计模型计算拟合了实验测得的口缓发质子能谱和布居到质子发射体子核不同终态的分支比，首次由实验数据出发初步指认了93Pd的基态自旋-宇称为9／2~±。同时与采用Woods-Saxon Strutinsky方法计算~(93)Pd的核位能面得到的结果进行了比较。计算结果支持对~(93)Pd基态自旋一宇称为9／2~+的实验指认。

CSRm内靶实验中的轻离子束流储存寿命研究

束流储存寿命对于储存环的建造和内靶实验都是一个很重要的参数。由于重离子冷却储存环工程的优化，HIRFL-CSR主环将能提供2．SGev的质子束流，这为强子物理研究提供了一个很好的平台。设计并建立一套针对强子物理的内靶系统己经列入到计划当中，与内靶相关的束流储存寿命研究也随之展开。本论文首先分析了在内靶实验中束流储存寿命的影响因素，即真空管道中的残余气体分子、冷却电子束和内靶，以及束内散射和集体效应等，并用理论解析和数值计算的方法，对各种因素的影响程度进行估算。研究表明，内靶散射影响下的束流储存寿命比其他因素导致的短2～3个数量级，内靶是影响束流寿命的决定性因素。其次，对CSRm将来实验中主要用到的Pelle七内靶和碳薄膜靶做了简要介绍，并计算了它们的有效靶厚大约为lx10、切ms／cmZ和5火1017atoms／CmZ。再者，用理论推导方法，对内靶的多次库仑散射和束流能量损失扰动对束流的影响进行了研究，推导了束流的横向和纵向发射度增长与束流每次打靶产生的小库仑散射角均方值气s和相对动量分散气了：之间的关系，并通过数值计算的方法给出了CSRm内靶实验条件的发射度增长曲线。最后，建立了内靶散射的MOnte-Carlo模拟程序，在模拟数据的基础上，总结研究束流的发射度增长规律，以及束流存储寿命与内靶厚度和束流能量的关系。计算表明，当存在Pellet靶（1、1016atoms／cm2）和c膜（5*1017 atoms／cmZ）时，2800Mev质子束的束流储存寿命分别为397秒和0．7秒，将来的内靶实验亮度大约为2 x 1033cm-2·s-1。

不同温度下氦离子辐照316L不锈钢氦泡形成的研究

本工作用2.5MeV的~4He~+分别在室温、500 ℃和600 ℃对经过固溶和冷扎处理的316L不锈钢进行了辐照，辐照剂量为2.7 × 10~(17)ions／cm~2，剂量率在3.6 × 10~(11) - 2.6 × 10~(12)ions／cm~2·s之间。用扫描电镜（SEM）观察样品表面形貌的变化，发现600 ℃时，辐照样品的表面出现许多形状不规则的小坑和类似颗粒的东西。用透射电镜（TEM）结合横截面制样技术观察样品内部氦泡的特征，发现室温和500 ℃下氦泡呈圆形，在600 ℃下氦泡呈多面体形状。温度由室温上升到500 ℃，氦泡的大小、数密度的变化比较小，当温度上升到600 ℃，氦泡直径迅速增大、数密度减小，估计在500 ℃和600 ℃之间存在一个氦泡演变转折点。对室温和600 ℃辐照样品中氦泡大小、数密度随深度的变化做定量测量，发现室温下氦泡的形核、长大主要依赖于氦原子的沉积浓度，而600 ℃下氦泡的形核、长大主要依赖于氦引进过程中产生的离位损伤（dpa）。另外，不同晶界处氦泡的特征也不同，大角晶界处氦泡优先生长；小角晶界处不存在氦泡的优先生长。在同一温度下，CW样品中氦泡的数密度比SA样品中氦泡的数密度大、直径小，对应氦泡产生的肿胀比SA样品的小

Preparation and performance of cellulose acetate/polyethyleneimine blend microfiltration membranes and their applications

A modified microfiltration membrane has been prepared by blending a matrix polymer with a functional polymer. Cellulose acetate (CA) was blended with polyethyleneimine (PEI), which was then crosslinked by polyisocyanate, in a mixture of solvents. In the membrane, PEI can supply coupling sites for ligands in affinity separation or be used as ligands for metal chelating, removal of endotoxin or ion exchange. The effects of the time of phase inversion induced by water vapor, blended amount of PEI and amount of crosslinking agent on membrane performance were investigated. The prepared blend membranes have specific surface area of 12.04-24.11 m(2)/g and pure water flux (PWF) of 10-50 ml/cm(2) min with porosity of 63-75%. The membranes, made of 0.15 50 wt.% PEI/CA ratio and 0.5 crosslinking agent/PEI ratio, were applied to adsorbing Cu2+ and bovine serum albumin (BSA) individually. The maximum adsorption capacity of Cu2+ ion on the blend membrane is 7.42 mg/g dry membrane. The maximum adsorption capacities of BSA on the membranes with and without chelating Cu2+ ion are 86.6 and 43.8 mg/g dry membrane, respectively. (C) 2004 Elsevier B.V. All rights reserved.

白桦光合特性的研究(英文)

测定了3年生白桦的光合与呼吸作用对温度,湿度以及CO2浓度的响应;还测定了光补偿点,光饱和点和CO2补偿点。结果表明:在目前的空气CO2浓度下,光合和呼吸作用的最适温度分别是24℃和30℃;当相对湿度是80%时,白桦能维持较强的光合作用;呼吸作用与相对湿度无明显的相关性;光补偿点和光饱和点分别是25 molm-2s-1和1375 祄olm-2s-1;CO2补偿点是180 礚 L-1;白桦在CO2浓度为2400 礚 L-1时仍有吸收潜力。图4参19。

白桦花期诱导技术的研究

在全光照(光合有效辐射尽可能保持在180μmolphotons·m-2·s-1以上)状态下,温度控制在25℃左右,湿度在60%以上,对塑料大棚中的白桦进行绞缢和CO2施肥处理,结果表明:绞缢是促进白桦提早开花的最有效措施,绞缢与对照两个水平间差异显著,绞缢开花率达38%,而对照开花率仅为2.9%。CO2施肥处理与绞缢处理之间不存在相互作用,CO2施肥不能明显使白桦提早开花。

长白山红松针阔叶混交林生态系统生产力的估算

利用LI-6400CO2分析系统测定了长白山红松针阔叶混交林生态系统土壤呼吸、乔木和灌木树干和枝条的呼吸、植物叶片光合与呼吸．同步监测森林小气候气象因子,建立土壤、树干、叶片与气象因子间的模型．根据红松针阔叶混交林植被群落特性,估算红松针阔叶混交林森林生态系统不同组分CO2通量．利用涡度相关技术监测红松针阔叶混交林净生态系统交换量．探讨温度、光合有效辐射对森林生态系统CO2通量的影响．通过分析发现,在当年的气候条件下,该森林净生态系统交换量主要受土壤呼吸和叶片光合的影响．红松针阔叶混交林净生态系统交换量全年变化范围在-4．67～13．80μmol·m-2·s-1．该森林生态系统CO2通量在冬季和夏季里平均分别为-2．0和3．9μmol·m-2·s-1(24 h平均值)．乔木、灌木和草本的初级生产力分别占阔叶红松林总初级生产力的89．7％,3．5％,6．8％．土壤呼吸是森林生态系统中最主要的CO2排放源,约占红松针阔叶混交林生态系统CO2排放的69．7％,植物叶片和枝干分别占15．2％和15．1％．在生长季和非生长季中红松针阔叶混交林净生态系统交换量分别占全年CO2通量的56．8％和43．2％．自养呼吸占总初级生产力的比值(Ra:GPP)为0．52(NPP:GPP=0．48)．森林生态系统地下当年碳积累量占总初级生产力的52％．土壤呼吸占总初级生产力的60％．红松针阔叶混交林NPP为769．3 gC·m-2·a-1．该森林净生态系统交换量(NEE)为229．51 gC·m-2·a-1．涡度相关技术获得的该森林生态系统NEE低于箱式法获得的19．8％．

长白山阔叶红松林主要树种及群落冠层光合特征

基于叶片尺度的光强-光合响应测定,结合冠层CO2涡度通量观测,研究了长白山阔叶红松林主要树种及群落冠层的光合特征．结果表明,叶片及冠层光响应过程均可以用非直角双曲线模型很好地表达．蒙古栎具有较高的光补偿点Lcp(28μmol·m-2·s-1)、光饱和点Lsp(>1800μmol·m-2·s-1)及最大净光合速率Pmax(9．96μmol·m-1·s-1),表现为典型的喜阳性特点;色木槭的表观量子效率α(0．066)最大,Lcp(16μmol·m-2·s-1),Lsp(800μmol·m-2·s-1左右)及Pmax(4．51μmol·m-2·s-1)最低,表现为弱阳性特点;红松针叶的α值显著低于阔叶树,但具有较高的Pmax,表现为半喜阳特点．在冠层,α和Pmax都位于温带森林报导值的上限,而Lcp位于下限．冠层光合特征参数与叶片具有较好的一致性,均表现为相对较高的光合能力,但环境胁迫,特别是高的饱和水汽压差可显著降低叶片和冠层的光合能力．

Attachment of marine sponge cells of Hymeniacidon perleve on microcarriers

Toward the development of an in vitro cultivation of marine sponge cells for sustainable production of bioactive metabolites, the attachment characteristics of marine sponge cells of Hymeniacidon perleve on three types of microcarriers, Hillex, Cytodex 3, and glass beads, were studied. Mixed cell population and enriched cell fractions of specific cell types by Ficoll gradient centrifugation (6%/8%/15%/20%) were also assessed. Cell attachment ratio (defined as the ratio of cells attached on microcarrier to the total number of cells in the culture) on glass beads is much higher than that on Cytodex 3 and Hillex for both mixed cell population and cell fraction at Ficoll 15-20% interface. The highest attachment ratio of 41% was obtained for the cell fraction at Ficoll 15-20% interface on glass beads, which was significantly higher than that of a mixed cell population (18%). The attachment kinetics on glass beads indicated that the attachment was completed within 1 h. Cell attachment ratio decreases with increase in cell-to-microcarrier ratio (3-30 cells/bead) and pH (7.6-9.0). The addition of serum and BSA (bovine serum albumin) reduced the cell attachment on glass beads.

东北地区农田防护林结构对林网内积雪分布格局的影响

东北地区冬季降雪是农田土壤水分的重要来源 .探索农田防护林结构对林网内积雪分布格局的影响 ,是经营实践中如何依据疏透度指标来指导农田防护林结构调控的关键问题 .通过由 3个不同疏透度林带组成的林网内积雪深度的测定 ,对农田积雪分布格局进行了研究 .结果表明 ,林网的结构对农田积雪分布产生较大影响 .疏透度不同的林网内积雪分布的空间格局有明显差别 ,而且疏透度差异越大 ,分布格局的差异越显著 .其中 ,在疏透度为 φ2w=0 .5 79、φ2s=0 .2 6 8的林网内 ,农田积雪分布比较均匀 ,总体上整个农田积雪深度较为一致 .这样 ,可依据疏透度与积雪分布格局的这种关系 ,指导冬季防护林带的结构调控与优化经营

非生长季长白山红松针阔叶混交林CO_2通量特征

采用开路式涡度相关系统对长白山红松针阔叶混交林非生长季的CO2通量特征进行连续监测。结果显示:非生长季CO2通量变动范围为-0·3~0·5mg·m-2s-1;秋末与初春均为显著的释放过程,虽然气温低于生物学最低温度,但在晴朗的午间,森林仍有数小时表现为碳汇的特征;在冬季覆雪状态下,森林存在微弱的相对恒定的CO2释放,在融雪阶段有一释放高峰;土壤温度高于0℃时,净生态系统碳交换量与5cm深土壤温度呈指数相关变化。观测期间(190d),长白山红松针阔叶混交林净碳交换量为127g C·m-2,整体表现为一定强度的碳释放。