BESⅢ主漂移室基于模式匹配的径迹重建

BESⅢ主漂移室径迹重建算法MdcPatRec, 是采用面向对象技术用C++开发的软件. 该算法使用模式匹配的方式寻找径迹段, 连接径迹段为径迹并进行最小二乘拟合. 使用模拟数据对算法进行了检验, 结果表明该径迹重建算法能够提供高的重建效率和好的动量分辨, 各项指标均达到设计要求. 同时具有好的抗噪声能力, 可以满足BESⅢ的使用要求.     

应用Kalman filter建立时间投影室的径迹重建算法

建立直线径迹模型,详细验证将其用于Kalman filter小型时间投影室径迹重建算法的正确性.结果表明径迹参数在一定的击中点下能够收敛到真实值.实际的径迹重建程序在MarlinTPC框架下实现.通过合理地选择径迹重建参数,程序能够有效地对噪声进行甄别并重建出径迹.本算法对大型时间投影室的径迹重建有借鉴意义.     

B介子工厂的挑战

 在近年的科技报章上,经常出现“B介子工厂”这个词语。那么,究竟什么是B介子工厂?为什么要建造B介子工厂?它对粒子加速器和探测器技术提出了什么样的挑战?这篇文章就来谈谈这些问题。 （一）什么是B介子工厂? 大家知道,高能物理研究作为构成宏观物质“大厦之砖石的“基本粒子”的结构及其运动规律。“基本粒子”不但非常微小(尺度在10^-子、米量级),而且除质子、中子、电子和光子等少数粒子以外,大多数只能在宇宙线中找到或在实验中产生,而且寿命都很短。要深入研究“基本粒子”的性质,就必须获取尽可能多的粒子事例。那么,这些粒子是如何在实验室中“生产”出来的呢?     

Improvements of The L3 TEC Track Resolution at Vertex

Two methods are used to improve the L3 TEC resolution at track vertex.First,refit the lepton tracks by constrained curvature from high precision measurements on electron energy and muon momenta. Second, correct the average value of track offsets in each half sector of TEC.Combined methods improve the lepton track resolution at vertex from 137μm to 60μm.     

北京谱仪Ⅱ顶点探测器径迹重建软件的研究

解决了北京谱仪Ⅱ顶点探测器径迹重建软件系统——VCJULI从HP-Unix平台到PC-Linux平台移植中“字典存放”和精度处理的问题,从而使两平台上的候选径迹差别从74%降至0.02%;径迹参数中一些量的差别从5%下降至0.5%左右.大大改善了寻迹质量并节省了CPU时间     

Fermion-Boson Vertex at Finite Chemical Potential

Based on the Ward-Takahashi identity at finite chemical potential and Lorentz structure analyms, we generalize the Ball-Chiu vertex to the case of nonzero chemical potential and obtain the general form of the frmionboson vertex in QED at finite chemical potential.     

考虑随机过程影响的径迹重建

对L3宇宙线实验中μ子事例的动量重建方法进行了研究.在事例的重建中,考虑了某些影响径迹重建精度的因素,如磁谱仪内部磁场的非均匀性和仪器自身物质对粒子的多次散射等过程引起的误差.经过修正后的μ子事例的动量分辨有了显著的改善.     

基于半导体制冷器的非均匀性校正

非均匀性是红外系统中影响图像质量的重要因素。为了更好地拟合探测器的响应曲线,充分发挥探测器的最佳性能,以获得良好的图像效果,在两点校正的理论基础上提出了一种更为实用的两点校正方法。通过单片机(MCU)控制半导体制冷器(TEC)以产生两个不同的校正温度点,系统分别读取在这两个温度点下所采集的两幅图像,利用两点校正算法计算探测器的响应率和暗电流。通过实验验证,这种校正算法实用,易于实现。     

Coupling Vertex of the Pomeron to Nucleon in QCD

The coupling vertex of the Pomeron to nucleon is derived from QCD. A γμ coupling vertex and coupling strength of β＝ 6.0 GeV-1, which has been used commonly as a free parameter in literature, are obtained. The result leads a support to the belief that the Pomeron could be a tensor glueball ξ(2230) with quantum numbers of IGJPC ＝ 0+2++ in nature.     

New Q Matrices and Their Functional Equations for the Eight Vertex Model at Elliptic Roots of Unity

The Q matrix invented by Baxter in 1972 to solve the eight vertex model at roots of unity exists for all values of N, the number of sites in the chain, but only for a subset of roots of unity. We show in this paper that a new Q matrix, which has recently been introduced and is non zero only for N even, exists for all roots of unity. In addition we consider the relations between all of the known Q matrices of the eight vertex model and conjecture functional equations for them.     

Integrals of Vertex Operators and uantum Shuffles

Given a braided vector space , we show that iterated integrals of operator-valued functions satisfying a certain exchange relation give rise to representations of the quantum shuffle algebra built on . Using the quantum shuffle construction of the 'upper triangular part' of a quantum shuffle, this provides a simple proof of the result of Bouwknegt, MacCarthy and Pilch saying that integrals of vertex operators acting on certain Fock modules give rise to representations of .     

A New Relativistic and Singularity Free Form Factor of Baryon Vertex

提出了一个新的、相对论的、无奇异点的重子顶点形状因子．这个形状因子满足强相互作用过程中,散射振幅从     

一个新的相对论的无奇异点的重子顶点形状因子

提出了一个新的、相对论的、无奇异点的重子顶点形状因子.这个形状因子满足强相互作用过程中,散射振幅从t道到s道变化的交叉对称性.