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高能重离子碰撞中K+/π+比例的显著升高被认为是夸克、胶子等离子体形成的一个可能信号.基于参加者核子模型和次级粒子形成时间的概念,本文对Si(14.5A GeV/c)与Au的中心碰撞进行了Monte Carlo模拟计算.在计算中考虑了如下次级碰撞过程:πN→K+Y、ππ→KK以及πN的单电荷交换反应.本文的计算结果表明:由这些次级碰撞过程导致的末态的K+/π+比例的升高不足以解释BNL的E802组观测到的实验数据. 相似文献
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π介子与周围核子发生次级碰撞可以改变K+/π+比.本文用Glauber模型计算在质子-核和核-核碰撞中的K+/π+比.计算表明,末态相互作用对K+/π+比的效应是重要的. 相似文献
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本文用自由的单胶子湮没机制和Hybrid中间态机制分别计算了π+-π-,K+-K-,K+-π-和K--π+之间的短程相互作用.计算结果表明,对于π+-π-散射,用hybrid中间态模型计算的结果能定性地符合实验,而对于K+-K-,K+-π-或K--π+相互作用,有待实验检验. 相似文献
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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. 相似文献
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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. 相似文献
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用一维粒子Code研究了旋转间断过渡层中的粒子轨道。发现绝大多数粒子都能穿过过渡层到达下游区;但是,有少量的粒子被捕获在过渡层内;也有一定数量的粒子被反射回上游区。捕获粒子数和反射粒子数与过渡层厚度D有关。在稳定旋转间断中,反射粒子数和捕获粒子数分别为2%和3%左右。对于不稳定的旋转间断,这两个比值可上升2-4倍。反射粒子和捕获粒子的动力学效应可以很好地解释旋转间断,中间激波和多重激波模拟的一些重要结果. 相似文献
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Rajendran Raja 《Pramana》2006,67(5):951-960
We describe the physics capabilities and status of the MIPP experiment which concluded its physics data taking run in March
2006. We show some preliminary results from this run and describe plans to upgrade the spectrometer. 相似文献
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流体—粒子模型及托卡马克等离子体稳态粒子流 总被引:2,自引:2,他引:0
基于俘获粒子与非俘获粒子对外力作用的响应截然不同,本文提出了一个简单而有效描述托卡马克等离子体响应特征的“流体-粒子”模型。 相似文献
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WU Weiliang CHEN Hanping 《Chinese Journal of Lasers》2002,11(1):45-50
1 Introduction Ifalightbeam passesthroughtheparticulatetransparentmedium ,itsintensitywillbeweakenedbecauseoftheextinctionofparticles[1] .Thisphenomenoniscausedbythescatteringandabsorptionof particles.Thescatteringelectromagneticwavesarediffusedinspaceal… 相似文献
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In this article a new receiving mode for scattering light by particle is theoretically discussed. Using this receiving mode the convex lens can be omitted during determining the extinction of particle. Therefore the extinction coefficient of sphere particles is redefined by extrapolating the conventional one. In terms of the calculation results of light scattering the definition of near-field extinction coefficient of a swarm particle is depicted. Through the error analysis it is proved that the error coming from the new definition of extinction coefficient is acceptable for engineering application. In addition, a technique for determining the particle size and density is presented in this article and the advantage using this receiving mode is described. 相似文献
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为了对比研究弱可压光滑粒子动力学(WCSPH)方法和不可压光滑粒子动 力学(ISPH)方法在模拟封闭方腔自然对流问题时的特性, 采用粒子位移技术有效地解决了高瑞利数条件下, 拉格朗日型SPH方法模拟封闭方腔自然对流时流体域内的粒子聚集和空穴问题, 将拉格朗日型SPH 方法求解封闭方腔自然对流问题的最高瑞利数提高到了106; 进而通过对比瑞利数分别为104, 105, 106的条件下, 采用拉格朗日型WCSPH、 拉格朗日型ISPH、欧拉型ISPH三种SPH方法模拟得到的封闭方腔速度分布云图、 温度分布云图、壁面努赛尔特数分布曲线和平均努塞尔特数, 分析了三种SPH方法在模拟封闭方腔自然对流时的精度、稳定性和计算效率. 结果表明: 在低瑞利数条件下, 以上三种SPH方法都可以较好地模拟此问题, 在高瑞利数条件下, 欧拉型ISPH方法的模拟结果最为精确; 拉格朗日型WCSPH方法模拟所得结果比拉格朗日型ISPH方法模拟所得结果稍好些.
关键词:
光滑粒子动力学
不可压光滑粒子动力学
粒子位移技术
自然对流 相似文献
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The collective diffusion of anisotropic particles in liquids plays a crucial role in many processes, such as self-assembly. The patchy particle, which is usually nearly spherical in shape, is an important anisotropic particle with different properties from other anisotropic particles like the ellipsoid liquid crystal particles. In the present study, molecular dynamics simulations are performed to study the collective diffusion of a two-dimensional anisotropic liquid system composed of Janus particles. The static structures and diffusion behaviours of anisotropic and isotropic Lennard-Jones liquids are compared. The long-time diffusion behaviour of an anisotropic liquid of nearly spherical Janus particles is found to be similar to that of an isotropic liquid because the orientation of the particles disappears over long-term averaging. The anisotropic properties of the Janus particles are mainly reflected in the spatial correlation of particle orientations and mid-time diffusion behaviour. The difference between nearly spherical anisotropic particles and rod-like particles is also discussed in this paper. 相似文献