排序方式: 共有20条查询结果,搜索用时 15 毫秒
1.
2.
研究了北京谱仪(BES)Ⅱ带电径迹测量误差矩阵的修正,使运动学拟合TELESIS方法在BESⅡ物理数据分析中得到应用.1)在BESⅡ数据重建程序中,加入了适当的MDC重建单丝分辨率(250μm)和Q修正.2)在TELESIS程序中,放入了BESⅡ有效物质量对BESⅡ误差矩阵进行多次库仑散射和dE/dX能损效应的修正.3)在此基础上,通过J/ψ→μ+μ-的数据样本分析,完成了BESⅡ24×106J/ψ事例RUN-by-RUN的误差矩阵刻度,同时对BESⅡMC数据也作了相应的刻度.经上述误差矩阵修正后,BESⅡ的TELESIS可以较好地满足BESⅡ数据分析工作的要求. 相似文献
3.
4.
本文在链近似下计算了QCD非微扰夸克和胶子完全传播子.我们仅考虑最低维非微扰效应即夸克凝聚<Ω│ψψ│Ω>和胶子凝聚<Ω│G2│Ω>对传播子的贡献,胶子凝聚通过作为<Ω│Aαμ(x)Abv(y)│Ω>在洛伦兹规范下展开级数的系数而引入.与采用固定点规范相比,胶子凝聚的引入没有破坏平移不变性.因而,我们计算出了夸克完全传播.如采用固定点规范不能做到这一点. 相似文献
5.
本文在背景场量子色动力学理论基础上考虑胶子凝聚对Goldstein方程的修正,并求出精确解.其解的行为表明简单的胶子凝聚图的贡献更有利于夸克和反夸克形成强子束缚态. 相似文献
6.
将在动量空间具有积分形式的单胶子交换梯形近似下Bethe-Salpeter方程化为微分方程,求出该方程在四动量为零时的赝标解全部分量,其中第一分量为已知的Goldstein解. 相似文献
7.
The Minimal Higgsless Model predicts the existence of new vector gauge boson W1± . By the process PP → W1± qq → W±Z0qq, Z0 → l+l-, W±→ qq (l=e,μ; q is hadronized to be jets), we study the sensitivity of searching for this possible vector gauge boson in the level of generator events of signal and backgrounds, then give integrated luminosity required to discover 5σ signal as a function of W1± mass. The generator for the signal PP→W1± qq→W±Z0qq at tree level is developed with the Minimal Higgsless Model and th... 相似文献
8.
In the LHC experiment, the neutral pions produced during jet fragmentation are the background sources for all physics channels with high-energy photons in their final state. In this paper, the application of the three-dimensional parametric formula for electromagnetic (EM) showers, which we developed in the Alpha Magnetic Spectrometer II experiment, is presented to distinguish the unconverted photons from the neutral pions. With the constructed electromagnetic calorimeter (ECAL) in a GEANT4 simulation, the parametric formulae were validated and the unconverted γπ0 discrimination was performed with the Toolkit for Multivariate Data Analysis (TMVA) package in ROOT for different transverse energies ranging from 15 GeV to 75 GeV, which is the most sensitive region for light Higgs (with mass ~120 GeV) searches with the channel H→γγ. With this discrimination method and the selected transverse energy region, we can reject π0 with the efficiency from ~40% (65--75 GeV) to ~90% (15--25 GeV) when keeping 90% γ efficiency. 相似文献
9.
10.