夸克-胶子等离子体中色屏蔽的时间演化与J/ψ、χ和ψ'压低

本文采用非相对论性禁闭势模型讨论了夸克-胶子等离子体中色屏蔽的时间演化和J/ψ、χ及ψ'的产额压低.     

矢量-标量混合禁闭势模型时的重夸克偶素

本文用考虑了相对论修正的势模型计算重夸克偶素的能谱、轻子宽度和辐射跃迁宽度. 在模型中我们假定: 矢量型禁闭和标量型禁闭同时存在, 在远距离标量型禁闭为主, 在近距离矢量型禁闭为主. 在这个假定下我们得到了与实验符合得较好的精细分裂值.     

通过基矢光前量子化方法对π介子的研究

为研究介子的性质,通过基矢光前量子化方法获得介子的光前波函数。基失光前量子化是一种在哈密顿量体系下基于量子场论的非微扰方法。在哈密顿量中我们考虑了动能项、基于全息色动力学的横向禁闭势、与横向禁闭势互补的纵向禁闭势和基于QCD的夸克-胶子相互作用。我们的基矢空间包括最低阶的两个Fock空间,即领头阶■与次领头阶■。根据所得的光前波函数我们计算了介子衰变常数以及(基于领头Fock空间的)电磁半径,这些结果与粒子数据手册(PDG)上的结果相近。此外,我们计算了(基于领头Fock空间的)介子部分子分布,QCD演化后,与原先的结果相近(蓝江山等,Phys Rev Lett,2 019,122:172 001.),能够很好地描述费米国家实验室(FNAL)与欧洲核子中心(CERN)的实验数据。     

重夸克偶素中的色屏蔽效应

将夸克-反夸克的禁闭位选为含有色屏蔽效应的禁闭势,计算了它对重夸克偶素cc和bb能谱的影响.与通常选用的线性禁闭势相比,含色屏蔽效应的禁闭势对ψ(cc)的高激发能级的轨道角动量可给出不同的预言,并且对ψ能级的轻子衰变宽度有明显的改进.     

手征–夸克耦合与双重子结构

运用SU(3)手征夸克模型,系统地研究了H,d*和d＇三个六夸克体系的结构,分析了SU(3)手征场和矢量耦合禁闭势等非微扰效应对三种六夸克态能量的影响.结果发现,SU(2)手征场的耦合,对形成六夸克态是有利的,但是扩大到SU(3)手征对称,则由于这些手征场的“云”,对六夸克系统形成束缚的双重子态起到了限制的作用,矢量耦合禁闭势有利于H的形成,而对d*则相反.     

夸克禁闭势与色Van der Waals力

本文采用高斯增长的夸克禁闭势和耦合道共振群方法研究了强子之间的色Van der Waals力问题. 先将两道耦合的微分方程组的边值问题转变为初值问题, 然后用基尔方法进行数值求解. 计算结果表明, 在高斯增长的禁闭势模型中不产生长程的色Van der Waals力. 这说明, 只要选择适当的夸克禁闭势, 则夸克势模型就既可用于描写强子的内部结构又能用来计算强子之间的相互作用力.     

LEP实验结果对大统一前子模型的限制

本文讨论了LEP关于轻中微子个数N_vN_{的实验结果对大统一前子模型的限制.由于LEP的精确实验结果有力支持了v}=3,可能的大统一前子模型为禁闭弱作用大统一前子模型.因此弱作用是禁闭的,它是前子之间超色作用的剩余效应.本文还讨论了若允许重中微子存在时,对大统一前子模型的限制.     

核环境中部分子演化与重组效应下的核内胶子分布

在既考虑到泄漏在束缚核子外的海夸克与胶子间的重组,又考虑到仍束缚在核子内的部分子由于其禁闭空间的变化而发生的演化的基础上,给出了核内胶子分布函数的普遍形式,并具体计算了锡梭与碳核的胶子分布比,结果与NMC实验合作组的最新实验相一致.     

在具有伸缩子的QCD势模型中的重介子

从伸缩子–胶子有效耦合理论得到的重夸克–反夸克势模型出发,计算了重介子的自旋平均能谱及轻子衰变和辐射跃迁宽度,并与Cornell势模型所得到的相应结果作了比较.结果表明,新的重夸克势的计算结果与重介子的实验数据更好地符合,而且估计的伸缩子质量5?7MeV很好地位于有关伸缩子质量的其他理论途径所估计的范围之内.     

重子谱中的中程相互作用及其对N-N核力的影响

本文基于夸克势模型, 在QCD单胶子交换势和禁闭的谐振子位势之上, 引入唯象的夸克中程势, 去拟合N≤2的非奇异重子谱. 结果表明: 适当形式的夸克中程势能使2GeV以下的重子谱与实验较好符合, 用此有夸克中程势的夸克位势我们还探讨了N-N相互作用.     

113Cd在0.01～20MeV能区中子诱导核反应的光学模型计算

基于核反应的光学模型和相应的实验数据,采用计算机自动调节势参数的方法,得到了中子入射¹¹³Cd能量为0.01～20Mev区间的一组光学势参数,并对实验数据少的核的光学参数调节方法进行了探讨。根据该参数对¹¹³Cd计算了中子诱导核反应弹性散射角分布和各种截面。理论计算值与实验数据符合很好。     

Theoretical Analysis and New Formulae for Half-Lives of Proton Emission

The proton radioactivity hMf-lives of spherical proton emitters are calculated by the cluster model with the con- tribution of a centrifugal potential barrier considered separately. The results are compared with the experimental data and other theoretical data, and good agreement is found for most nuclei. In addition, two formulae are pro- posed for the proton decay half-life of spherical proton emitters through the least squares fit to the experimental data available, and could reproduce the experimental half-lives successfully.     

A continuum thermal stress theory for crystals based on interatomic potentials

This paper presents a new continuum thermal stress theory for crystals based on interatomic potentials.The effect of finite temperature is taken into account via a harmonic model.An EAM potential for copper is adopted in this paper and verified by computing the effect of the temperature on the specific heat,coefficient of thermal expansion and lattice constant.Then we calculate the elastic constants of copper at finite temperature.The calculation results are in good agreement with experimental data.The thermal stress theory is applied to an anisotropic crystal graphite,in which the Brenner potential is employed.Temperature dependence of the thermodynamic properties,lattice constants and thermal strains for graphite is calculated.The calculation results are also in good agreement with experimental data.     

Decay rates and electromagnetic transitions of heavy quarkonia

The electromagnetic radiative transition widths for heavy quarkonia,as well as digamma and digluon decay widths,are computed in the framework of the extended harmonic confinement model(ERHM) and Coulomb plus power potential(CPP_v) with varying potential index v.The outcome is compared with the values obtained from other theoretical models and experimental results.While the mass spectra,digamma and digluon widths from ERHM as well as CPP_(v=1) are in good agreement with experimental data,the electromagnetic transition widths span over a wide range for the potential models considered here making it difficult to prefer a particular model over the others because of the lack of experimental data for most transition widths.     

Accurate He-Ag(110) interaction potential determination by selective adsorption

The first accurate energy level measurements of a He-metal interaction potential are reported for the Ag(110) surface as obtained from selective adsorption data. The fitting of the experimental data with a suitable phenomenological potential leads to a well depth of 6.0 ± 0.1 meV. The potential curve is considerably softer than those obtained for He interaction with either insulators or semiconductors and is in good agreement with theoretical predictions.     

Structural phase stability and elastic behavior of III-V scandium pnictides

A modified interaction potential (MIPM) model (including the covalency effect) has been developed and applied for the first time to investigate the high-pressure structural phase transition of scandium pnictides (ScAs and ScSb). Phase transition pressures are associated with a sudden collapse in volume indicating the occurrence of first order phase transition. The phase transition pressures and associated volume collapses obtained from present potential model show a generally better agreement with available experimental data than others. The elastic constants and their pressure derivatives are also reported. Moreover, the thermo physical properties have also been obtained successfully. Our results are in good agreement with available experimental and theoretical data.     

Molecular Dynamics Simulations of the Elastic Anisotropy of Pd at Extreme Conditions

It is very interesting to discover the elastic properties of engineering material palladium, especially its elastic anisotropy along Hugoniot states. We here investigate the evolution of its high pressure and temperature(PT) elastic ansotropy along Hugoniot using molecular dynamics simulations based on accurate classical interatomic potential. In order to testify the validity of the interatomic potential of Pd in describing the high PT elastic properties, we calculate its isothermal and adiabatic elastic moduli using molecular dynamics method. The obtained data are in good agreement with experimental data. From the isothermal elastic constants, we deduce the Hugoniot acoustic velocities and find that the resulting data are in good agreement with experimental acoustic velocity data. Based on the reliable elastic constants, we further investigate the spacial elastic ansotropy along Hugoniot PT states. It is found that the spacial elastic anisotropy of Pd increases along Hugoniot states.     

中子与116,118,120,122,124Sn反应非弹性散射的理论计算和分析

应用现有的中子与原子核Sn及其同位素反应的总截面,去弹性散射截面,弹性散射截面和弹性散射角分布的实验数据,获得一组普适的中子与Sn及其同位素反应的光学模型势参数.利用这组光学模型势参数,扭曲波玻恩近似理论,核反应Hauser-Feshbach理论和预平衡反应的激子模型,计算和分析了中子与^{116,118,120,122,124}Sn反应分离能级的非弹性散射截面和角分布.理论计算与实验数据进行了分析比较.     

New Investigations on Meson Spectra Based on the Relativistic Equation for qq Bound States

By considering the retardation effect of gluon propagation and a general Lorents structure of the confinement, a retarded and off-shell one-gluon exchange potential and a harmonic oscillator-dominant confining potential with a certain relativistic corrections are derived based on the relativistic Pauli-Schr6dinger equation for quark-an tiquark bound states. Use of these potentiale to caJculate meson spectra leads to the results which are in good agreement with the experimental data.     

考虑热效应的Vinet状态方程及其应用

 基于爱因斯坦模型将Vinet等人提出的关于金属固体的通用物态方程推广到包括热效应。采用最近邻普遍化Lennard-Jones势描述金属离子之间的有效配对相互作用,将每个离子的势能展开为离子位移的二阶泰勒级数,从而推导出爱因斯坦温度和Grüneisen常数的解析表达式,该表达式只与体积有关而与温度无关。推广方程包括的7个参数只有5个是独立的,在高于德拜温度时,只需要4个参数。对典型金属及两种非金属材料计算的结果与实验符合得很好。