手征性硫代磷酸及其衍生物的研究(Ⅰ)——O-乙基-O-苯基硫代磷酸的拆分及其手征性硫(醇)代酯的合成

以奎宁为拆分剂,在甲醇溶液中,将O-乙基-O-苯基硫代磷酸(Ⅰ)拆分成一对对映异构体。     

离散型固体力学及其间断型变分原理

本文对即将形成的一门新的学科——离散型固体力学的基本假设,微分形式的方程,及其间断型变分原理进行了论述.离散型固体力学是离散介质力学的一个分支,是近期以来力学的一个发展方向.它是基于固体体系具有离散性、可分性,待解函数在定义城内具有各种不同的间断性,以及定义域的边界可动性的基础上,为解决种种情况下的固体的应力,位移、应变所形成的力学系统.当待解函数在整个定义域内为充分光滑的函数类和略去边界可动性的影响时,则离散型固体力学就退化为连续介质力学范畴的古典固体力学.它所属的变分原理,在相应的情况下,也就退化为古典与非占典变分原理.     

有限元广义伽略金方程,边界变分方程,边界积分方程

在[1]的基础上,我们进一步应用可动边界的变分原理于固体体系的离散分析,得到有限元广义伽略金方程,边界变分方程,边界积分方程.这些方程描述了待解函数在元素内部与元素的边界上应满足的方程.当对固体体系进行离散分析时,可以应用这些方程去建立不同情况下的求解待解函数的离散方程.亦可作为相应情况下的简化计算的依据.由本文得到的边界积分方程可知,在[2]中提出的J积分形式,应用于内部元素边界的围道积分计算是不适宜的.     

Solid mechanics of discrete form and the variational principles of the discontinuous form

This paper discusses the fundamental assumptions,the differen-tial equations,and the variational principles of discontinuousform belonging to a new developing branch of science-the solidmechanics of discrete form.The solid mechanics of discrete formbelongs to the branch of science of discrete medium mechanicswhich is the developing direction of the mechanics for the pre-sent.Based on the solid system with discretization and sepa-rability,the unknown functions with discontinuity in definedregions and the defined regions with variable boundaries,themechanics systems to solve the solid displacements,strains andstresses in various cases are called the solid mechanics of dis-crete form.when the unknown functions are sufficiently smooth func-tions in the whole defined region and the effects of the vari-able boundaries are disregarded,the solid mechanics of discreteform will degenerate into the classical solid mechanics belong-ing to continuum.mechanics:Its variational principles will de-generate into the clas     

双奇核中π1/2－[541]⊙νi13/2带的系统学特征

通过束流能量为97MeV的¹⁵²Sm(¹⁹F,5n)¹⁶⁶Lu熔合蒸发反应,用在束γ(谱学方法研究了¹⁶⁶的高自旋态,建立了5条转动带,其中3条带是本实验中首次确定的.发现了π1/2^－[541]⊙ν5/2⁺[642]带的低自旋旋称反转现象,该带的反转点自旋值17.5h同A=170区奇奇核的π1/2^－[541]⊙νi_13/2带的反转点变化趋势非常相符.     

激光诱变滇"三角大香糯"的遗传效应研究

2 0 0 1年我们用He -Ne激光辐照加电场、磁场激发对滇“三角大香糯”进行了育种研究〔1〕,并得到了五株有较优变异的稻种 (第 1代M1 )。 2 0 0 2年我们种植了这五株稻种 ,并进行了各生育期的田间试验观测。分析了诱变滇三角香糯育出稻种的遗传性质     

级联弧放电氦等离子体特性研究

采用另加偏压的单阴极弧氦放电直线等离子体装置对氦等离子体的基本特性进行了研究。对氦轴向输运规律做了描述并与光谱测量数据做了定性地比较。实验结果表明,氦等离子体的电子温度与电子密度均随放电电流、约束磁场的增加而增加。氦原子与氦离子的辐射光谱随放电电流、偏压、磁场的变化规律进行了测量分析,同时氦离子对钨靶积分辐照效应进行了观察。这些结果不但提供了氦等离子体的基本特性,对于研究氦离子与面向等离子材料相互作用导致产生气泡、肿胀、脆化损伤等的评估,特别是对将来伴有(n, α)反应时具有一定的参考价值。     

20Mgβ衰变谱学与15O(α,γ)19Ne反应(英文)

15O（α,γ）19Ne（p,γ）20Na反应链是高温CNO循环向快速质子俘获过程突破的一条关键路径,相关的反应率输入量可通过20Mg的β衰变可布居19Ne共振态并测量其衰变性质来获得。通过高效率高精度地测量20Mg β衰变中产生的质子与γ射线得到了20Mg衰变的详细信息,并构建了完整的衰变纲图,还进行了19Ne 4 033 keV共振态衰变性质的探索,获得了该态在20Mg β衰变中被布居的分支比上限。通过比20Mg和20O镜像能级跃迁的结果确认了同位旋非对称性,为检验相关理论模型提供了精确的实验数据。对于突破路径中有重要影响的19Ne 4 033 keV共振态的性质,有待更高统计的实验进一步研究。The breakout from the hot CNO cycle to the rapid proton capture process can occur via the 15O(α,γ)19Ne(p,γ)20Na reaction sequence, and the β decay of 20Mg can be used as an alternative method to characterize some specific resonances, which will provide detailed nuclear structure input for reaction rate calculations. The reliable information on the decay properties and structure of 20Mg was obtained by measuring the emitted particles and γ-rays in the β decay with high efficiency and high resolution. Attempt was also made to search for the decay channels associated with the 4 033 keV resonance in 19Ne. To test fundamental symmetries, the transitions in the mirror decays of 20Mg and 20O were compared. The precise experimental data presented here would be important to constrain the theoretical calculations. It is desirable to clarify the astrophysically relevant problem by further experiments with improved statistics on the basis of the present work.     

硅探测器的数字化脉冲形状甄别

介绍了利用硅探测器的脉冲形状甄别进行粒子鉴别的原理。详细叙述了基于数字化方法的脉冲形状甄别的实现。采样频率和位数是数字化方法的两个重要参数。对于硅探测器信号,采用100 MS/s,12 bit的Digitizer可以满足脉冲形状甄别法对时间分辨的要求。同时对该方法粒子鉴别的特征和能量阈值做了简要的分析和对比。粒子背面入射硅探测器的所得的阈值低于正面入射的情况。例如对于氖周围的同位素,背面入射情况的阈值约为100 MeV,为正面入射情况下鉴别阈值的二分之一,相当与ΔE-E方法中ΔE探测器厚度约为60 μm情况下的阈值。最后定性讨论了硅探测器的电阻率不均匀性和沟道效应对粒子鉴别性能的影响。In this paper Pulse Shape Discrimination(PSD) for silicon detector has been briefly introduced. The emerging digital method successfully applied to detector signal processing makes digital PSD method one of the most promising particle identification methods. Sampling frequency and the number of bits are two key parameters of digital method. For silicon detector signal, adopting 100 Ms/s, 12 bit Digitizer can satisfy the time resolution requirement of PSD method. The identification characteristic and energy threshold of this method have been discussed and compared with both front injection and rear injection cases. Energy threshold with rear injection usually is much lower than that with front injection. For example, around for Neon isotope energy threshold with rear injection is about 100 MeV which is only half of the threshold with front injection, also equivalent to thickness of about 60 μm silicon detector threshold in ΔE-E method. At the end the impact of silicon detector's resistivity nonuniformity and channel effect on the identification capacity of PSD method has been discussed in detail.