电子和X射线激发原子核

本文研究了关於电子激发原子核的理论。对当原子核由於各多极核矩和电子的电磁相互作用而引起的激发截面进行了一些估计,并且导出表示电子和X射线对原子核激发现象相互关系的公式。这公式仅是原子核能级跃迁中的能量、角动量、和宇称的函数,而不因其他原子核性质而变。把理论的结果和激发In¹¹⁵的试验测量作了一些比较。不过因为缺乏充分的实验测量数据,没能从这比较上得到肯定的结论。於是建议了一些可能进行的研究原子核能级的试验方法。     

奇异粒子的性质及其产生和衰变

用一架30厘米×30厘米×10厘米磁场为6200高斯的云室,在海拔3185米的云南落雪高山实验室拍摄了30000对照片,获得105个V⁰,而可以进行分类的有43个。其中有26个θ₁⁰,16个Λ⁰和一个θ₂⁰。本文对θ₁⁰,Λ⁰和一个θ₂⁰进行了研究,其结果如下:1)Q值,Q_(Λ⁰)=(36.2±2.5)Mev,Q_(θ1⁰)=(233±11)Mev;2)平均寿命,τ_(Λ⁰)=(3.19_-0.92^+2.42)×10^-10秒,τ_(θ1⁰)=(1.14_-0.27^+0.49)×10^-10秒;3)动量分布与以前的工作没有显著差别;4)N(Λ⁰)/N(θ₁⁰)=0.51±0.22(权衡数);5)Λ⁰和θ₁⁰在质心系的衰变角分布没有明显的不对称性;6)一个θ₂⁰在静止坐标系寿命为～10^-9秒,衰变类型可能为θ₂⁰→π^-+π⁺+π⁰或者θ₂⁰→π^±+μ^?+ν。     

K+介子衰变的分枝比

The branching ratio of the following three modes of K⁺-meaon decay K⁺→μ⁺+π⁰+ν K⁺→e⁺+π⁰+ν K⁺→μ⁺+ν is calculated by using the theory of the universal Fermi weak interaction proposed by Feymann and others. Perturbation method with cut-off is used. The ratio obtained is 1:1.5:12, which is in fair agreement with the experimental value 1:1:15. It is shown, other conbinations of Fermi interactions can not give result in agreement with experiment.     

各向异性高压物质的电子能谱

本文以高压物质作为一种简单的各向异性金属模型,研究了静晶格场、电子间库仑相互作用和通过声子场的相互作用对单粒子元激发谱的影响。讨论了周期场中电子格林函数的微扰论级数,原则上解决了用微扰论求周期场中费米系统能谱的问题。具体计算了面心立方和体心立方高压物质的费米面和态密度,给出了数值结果。     

变容管的非线性性能及时变参量的分析

在变容管的各种参量应用中,变容管的非线性性能成为最基本的重要资料。提高变容管的非线性度,在应用中可以相应减小注入功率。在研究低注入或其他非正弦波注入应用的特性时,更应对变容管时变参量的基波及谐波分量与变容管非线性度及注入电压比等之间的关系深入研究。本文目的在于分析上述问题,选用合适的非线性性能的表示法,采用图解法求出变容管归一化时变参量的基波及谐波分量的特性,并绘出这些分量与变容管非线性度γ,注入电压比m₁之间的关系曲线。这些通用曲线在分析变容管的各种参量应用中可作为重要参考资料,并举例示出这些曲线的用途。     

6.8GeV/cπ-N非弹性作用下π0介子的产生

利用联合原子核研究所24立升丙烷气泡室照片,对动量为6.8GeV/cπ^-介子与核子非弹性作用产生π⁰介子的问题进行了研究。扫描了约2700对立体照片。在宽度为29.3厘米的有效范围内得到了1275个π^--N非弹性作用事例。在936个π^--p事例和339个π^--n事例中,观察到正电子、负电子对数目分别为240和89。考虑了气泡室对γ光子的探测效率,我们得到每个事例产生的平均π⁰介子数n_(π⁰)=1.00±0.06。γ光子的平均横动量为p_⊥γ=173MeV/c。此外,着重研究了γ光子的能量分布。在γ光子全部是由π⁰介子衰变产生以及π⁰介子和π^±介子具有相同能谱的假设下,利用在相同入射粒子能量的π^--N作用中所产生的次级π^±介子能量分布变换成γ光子的能量分布;将本实验所得的γ光子能量分布和变换得到的分布进行比较,这两个分布在实验误差范围内完全符合。     

晶粒取向镍—铁合金各向异性的磁转矩法研究

本文测定了冷轧的及冷轧后又经不同温度退火的50％Ni-50％Fe合金的磁转矩曲线,从而对试样中的冷轧及再结晶结构作了推断。从具有完整立方结构的试样上测得的磁晶各向异性常数k₁和其他作者从单晶体上得到的值相近,而从保有冷轧结构的试样定得的k₁值则较大。考察了影响k₁测定值的可能因素;讨论了磁致伸缩各向异性导致的弹性能以及有序程度对k₁值的影响。 关键词：     

Effects of Impurity on the Ground—State Transitions of a Quantum Dot in Strong Magnetic Field

The low-lying spectra of parabolic quantum dots with or without an impurity at the center are investigated.While it has been known that the electron-electron interaction leads to ground-state transitions on magic values of angular momentum in a magnetic field.We show,in this paper,that the implantation of an impurity ion at the center can either enhance or suppress such transitions,depending on whether it is an acceptor or a donor ion.     

Realization of Tip Tilting By 8-Step Line Tilting

By direct calculation of rotation matrices of SO(3), we show how certainspecific sequence of eight consecutive rotations of digital angles can yielda tilting of a facet mirror. We also design a detailed program specificallyto tilt an array of mirrors from planar orientation to the required focusingorientation. We describe how to use the 8-step to realize the focusing ofthe mirror array. We have found, in our designed program, an importantfeature of row-sharing during the rotations for the columns and similarlythe column-sharing during the rotations for the row. This feature can save alot of operating time during the actual realization of the mechanicalmovements.     

A Prediction of a New Dibaryon System (Ω-Ω-)Jπ=o+

The structure of a new dibaryon (ΩΩ)_o+ is studied and predicted in the framework of the chiral SU(3) quark model by solving a resonating group method equation. The binding energy of this dibaryon is around 100 MeV, the mean root square of the distance between two Ωs is 0.84 fm and the preliminary estimated mean lifetime is about two times longer than that of the free Ω. All these interesting properties and also the two negative charge units it carried could make it be easily identified experimentally in the heavy-ion collision process. The production probability of this new dibaryon in 158A GeV Pb+Pb collision is estimated using the thermal model, which is of the order of 10^-6 to 10^-5 per event; And it is expected, that with the increase of temperature, the production rate will also be increased.