π+介子辐射衰变分枝比

本文应用标准微扰方法计算π介子衰变过程中π⁺→e⁺+v+r对π⁺→μ⁺+v的分枝比。文中应用了V-A型普适费米弱作用及沙拉姆提出的强作用,计算结果与目前实验结果没有矛盾。     

K+介子的三体轻子衰变

本文利用色散关系方法,假设普适V-A弱相互作用和奇异矢量流不守恒,从而对形状因子f₀,f₁的色散关系进行一次减去,计算了K_μ3⁺、K_e3⁺衰变中的π⁰能谱,K_μ3⁺衰变中的μ⁺能谱和μ⁺的纵向极化。计算中只考虑了K₁^*(m_*=888MeV)中间态对色散积分的贡献。参数σ取为+2.1的结果和实验在误差范围内相符合。放弃奇异矢量流部分守恒假设与实验符合的程度比保持这一假设要好一些。     

K~ 介子衰变的分枝比

一.引言 费曼和盖尔曼以及马夏克和森德香同时提出了费米子之间的普适弱相互作用的理论。将这一理论应用于β衰变现象以及一些其他的弱相互作用现象的研究,得到了很好的结果。将这一理论应用到更多的弱相互作用现象的研究中去是有意义的。我们在本文中以这一理论为基础,讨论K~ 介子下列三种方式的衰变     

关于K+介子和核子的弹性散射

本文用塔姆-唐可夫近似解K⁺介子和核子的弹性散射问题,得到了K介子实验室动能400Mev以下的相移截面和能量的关系,并和实验及前人的理论结果作了比较。计算中较严格考虑了核子反冲效应,指出了在考虑了反冲效应后能使理论曲线在高能端更与实验曲线接近。同时就Λ-K和∑-K的各种可能的宇称情况进行了分析,排斥了相对宇称皆正的可能,并指出Λ-K和∑-K的相对宇称选取不同的符号和二者皆取负号一样,能符合K⁺-p散射实验,但在分析K⁺-n散射时仍遇到困难。     

π~ 介子辐射衰变分枝比

本文应用标准微扰方法计算π介子衰变过程中π~ →e~ v r对π~ →μ~ v的分枝比。文中应用了V-A型普适费米弱作用及沙拉姆提出的强作用,计算结果与目前实验结果没有矛盾。     

非因子化方法研究D+→K0K+衰变

在领头阶和αs 修正阶,用QCD因子化方法,并对它的软胶子效应用光锥QCD求和规则分析D⁺→K⁰K⁺衰变过程,我们分析发现朴素因子化方法的结果远离实验结果,QCD因子化方法结果靠近实验结果,但是,在QCD因子化方法中,若考虑软胶子效应,其结果与实验结果相一致.另外,计算发现,软胶子效应在该衰变道中有相当大的贡献,因此不能被忽略     

再散射输运模型与K+/π+比的系统学

用含再散射效应的简单的强子输运模型,研究了AGS能量(14.6AGeV/c)下p+p、p+Au和Si+Au反应的K⁺/π⁺比值,再现了该比值由P十P到Si十Au不断增长的实验事实.CERN能量(200AGeV/c)和AGS能量下,K⁺/π⁺比值相近的实验事实也得到了解释.     

Z0衰变产生Bc介子

本文基于最重要的"硬"产生机制,计算了Z⁰衰变产生B_c(或B_c)介子并伴有c(或c)和b(或b)两个重夸克喷注的产生率.指出在LEP上的下一次取数据中将产生出足够数目的B_c(或B_c)介子的性质成为可能.     

高能核碰撞中的K+/π+比与次级碰撞效应

用程函近似分析在高能核碰撞中次级作用对K⁺/π⁺比的影响.计算表明,在K⁺/π⁺比中次级碰撞效应是重要的.     

相对论性重离子碰撞中次级碰撞对K+/π+比的影响

本文基于参加者-旁观者模型,用Monte Carlo方法分析了相对论性重离子碰撞中各种次级碰撞对K⁺/π⁺比值上升的影响.结果表明,公认仅考虑次级碰撞不足以解释实验观测的K⁺/π⁺比值上升.     

K^＋—核散射研究进展

本简要回顾了K^ -核散射实验和理论方面近几年的研究进展。我们通过把介质中的K^ -核子相互作用与介质中的夸克凝联系起来,计算了K^ -核相互作用的非传统机制的贡献。结果表明核密度相关的介质内夸克凝聚可以解释K^ -核散射中的非传统介质效应。     

Measurement of the reactions K+d → K+d and K+d → p+pn and an investigation of elastic K+-nucleon scattering at 4.6 GeV/c

The coherent elastic reaction K⁺d → K⁺d and the break-up reaction K⁺d → K⁺pn are studied in a K⁺d experiment at 4.6 GeV/c which the CERN 2 m bubble chamber. Partial and differential cross sections are given and the slopes of the differential cross sections are determined. The results for the reaction K⁺d → K⁺p(n_s), where n_s denotes the spectator neutron, are compared with those of the reaction K⁺p → K⁺p on free protons. Combining our data with existing data on the reactions K⁺d → K⁰pp and K⁺p → K⁺p, parameters of the elastic K⁺-nucleon scattering at 4.6 GeV/c are determined in the framework of the Glauber model. The D-wave of the deuteron and spin-flip effects are taken into account.     

场流关系和π+→e++ν+γ的衰变过程

本文应用由复合场场论或场代数导出的轴矢流的场流恒等式计算了π介子的辐射衰变π⁺→e⁺+ν+γ过程。计算结果与目前的实验大致相合。     

A spin-parity analysis of the K+K+K− system produced in the reaction K+p → K+K+K−p

We present the first spin-parity analysis of the K⁺K⁺K^?) system produced in the reaction K⁺p → K⁺K⁺K^?p, and show that the general features of this system resemble those of the (ππ⁺π^?) and Kπ⁺π^?) systems produced in the reactions π(K)p → π(K)π⁺π^?p. There is a low mass enhancement, (47 ± 11)% of which corresponds to 1⁺ states decaying to Kø. At higher (K⁺K⁺K^?) masses 2^? → Kf′ becomes increasingly significant and at all masses there is a 0^? contribution of roughly 30%.     

范德瓦耳斯分子K39Xe129中的自旋-转动对自旋交换耦合常数之比的确定

光泵的方法被用来确定K³⁹Xe¹²⁹范德瓦耳斯分子中的自旋-转动耦合常数对自旋交换耦合常数的比值X。详细地讨论了这些测量理论。得到比值X=γN/α=4.8(1)。 关键词：     

S-P wave interference in K+K− photoproduction near K+K− threshold

A mass-dependent asymmetry was observed in the decay angular distribution of a photoproduced K⁺K^? system near the K⁺K^? threshold. The corresponding moments 〈Y₁⁰〉 have been evaluated. Interpreting the asymmetry as an S-P wave interface due to the states S₉₉₃¹(0⁺) and ø₁₀₁₉(1^?) one can compute the moments 〈Y₁⁰〉 through an amplitude analysis. The theoretical calculation reproduces the experimental results well, if one assumes a real S-wave amplitude for the S₉₉₃¹. The data cannot be explained by a non-resonant real S-wave. Other possibilities have been discussed. An estimate of the photoproduction cross section of the $\text{S}{}^1\text{→}\text{K}{}^{\mathrm{+}}\text{K}{}^{\mathrm{?}}$ can be given on the basis of the above hypothesis.     

Particle exchange in K+p scattering

Recent phase-shift analyses of K⁺p scattering have shown many features of particle exchange. In exotic channels, particle exchange appears to play a more prominent role than in non-exotic channels where exchange are obscured by direct channel resonances. In the present paper particle exchange has been investigated in the momentum range 0.9 to 1.5 GeV/c, using a phase-shift analysis in which coupling constants were available parameters.     

The K+π- elastic scattering cross section as observed in K+p→K+π-Δ++ from 3 to 13 GeV/c

The four-body reaction K⁺p→K⁺π^-Δ⁺⁺ is analysed in a sample of 77 300 bubble chamber events of K⁺p→K⁺π^-π⁺p for beam momenta from 2.5 to 12.6 GeV/c to study the K⁺π^- elastic scattering cross section. The relative merits of several analytic continuations to the pion pole are discussed. Maximum likelihood method is used and, for each experiment fits are performed simultaneously over the whole range of the M(pπ⁺), m(K⁺π^-) and t variables. The K⁺π^- cross section is parametrized in terms of the down solution for the s-wave, a p-wave resonating at the K¹(890) and a d-wave resonating at the K¹(1420). Fitted values are obtained for the four-body cross section, the s-wave contribution to the K⁺π^- cross section, and the masses and widths of the K¹(890) and K¹(1420).