首页> 外文学位 >First measurement of the ratio of branching fractions Br(lambdab to lambdac mu nu)/Br(lambdab to lambdac pi) at CDF II.
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First measurement of the ratio of branching fractions Br(lambdab to lambdac mu nu)/Br(lambdab to lambdac pi) at CDF II.

机译:在CDF II上首次测量分支分数Br(lambdab与lambdac mu nu)/ Br(lambdab与lambdac pi)之比。

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摘要

We present the first measurement of the ratio of branching fractions B&parl0;Lb→L+ cm-n&d1; m&parr0;/B&parl0;Lb→ L+cp-&parr0; based on 171.5 pb-1 of pp¯ collisions at s = 1.96 TeV taken with the CDF-II detector. In addition, we present measurements of B&parl0;B0→D*+ m-n&d1; m&parr0;/B&parl0;B0 →D*+p-&parr0; and B&parl0;B0→D+m -n&d1;m &parr0;/B&parl0;B0→D +p-&parr0; , which serve as control samples to understand the data and Monte Carlo used for the Lb analysis. We find the relative branching fractions of the control samples to be: B B0→D* +m-nm B B0→D *+p- =17.7+/-2.3stat +/-0.6syst +/-0.4BR +/-1.1UBR, and B B0→D+ m-nm B B0→D +p- =9.8+/-1.0stat +/-0.6syst +/-0.8BR +/-0.9UBR, which are consistent with the ratios obtained by the Particle Data Group at the 0.7 and 1.1 sigma level, respectively. Finally, we obtain the relative Lb branching fraction to be: B&parl0;L b→L+cm- n&d1;m&parr0; B&parl0;Lb→L +cp-&parr0;=20.0 +/-3.0stat+/-1.2 syst+0.7-2 .1BR +/-0.5UBR. The uncertainties of the three relative branching fractions are from statistics, CDF internal systematics, external measured branching ratios and unmeasured branching ratios, respectively. We present a method to derive B&parl0;Lb→L+ cp-&parr0; using previous CDF measurements and obtain B&parl0;Lb →L+cp-&parr0; =0.41+/-0.19stat⊕syst +0.06-0.08&parl0;PT&parr0; %, where the last uncertainty is due to the measured Lb PT spectrum. Combining B&parl0;Lb→L+ cp-&parr0; with our result, we determine the exclusive semileptonic branching fraction for the Lb ; B&parl0;Lb →L+cm- n&d1;m&parr0;= 8.1+/-012stat+1. 1-1.6syst +/-4.3&parl0;B&parl0;Lb→ L+cp-&parr0;&parr0; %.
机译:我们提出了支化分数B&parl0; Lb→L + cm-n&d1;的比率的首次测量。 m&parr0; / B&parl0; Lb→L + cp-&parr0;基于CDF-II检测器在s = 1.96 TeV时pp碰撞的171.5 pb-1的结果。另外,我们给出了B&parl0; B0→D * + m-n&d1;的测量值。 m&parr0; / B&parl0; B0→D * + p-&parr0;和B&parl0; B0→D + m -n&d1; m&parr0; / B&parl0; B0→D + p-&parr0; ,用作控制样本以了解数据以及用于Lb分析的Monte Carlo。我们发现对照样品的相对分支分数为:B B0→D * + m-nm B B0→D * + p- = 17.7 +/- 2.3stat +/- 0.6syst +/- 0.4BR +/- 1.1UBR和B B0→D + m-nm B B0→D + p- = 9.8 +/- 1.0stat +/- 0.6syst +/- 0.8BR +/- 0.9UBR,这与通过粒子数据组分别处于0.7和1.1 sigma级别。最后,我们得到相对的Lb分支分数为:B&parl0; L b→L + cm- n&d1; m&parr0; B& Lb→L + cp-&parr0; = 20.0 +/- 3.0stat +/- 1.2 syst + 0.7-2 .1BR +/- 0.5UBR。这三个相对分支分数的不确定性分别来自统计学,CDF内部系统学,外部测得的分支比和未测到的分支比。我们提出一种导出B&parl0; Lb→L + cp-&parr0;的方法。使用先前的CDF测量值并获得B&parl0; Lb→L + cp-&parr0; = 0.41 +/-0.19stat⊕syst+ 0.06-0.08&parl0; PT&parr0; &percnt ;,其中最后一个不确定性是由测得的Lb PT频谱引起的。合并B&parl0; Lb→L + cp-&parr0;根据我们的结果,我们确定了Lb的排他性半轻体分支分数; B& Lb→L + cm-n&d1; m&parr0; = 8.1 +/- 012stat + 1。 1-1.6syst +/- 4.3&parl0; B&parl0; Lb→L + cp-&parr0;&parr0; %。

著录项

  • 作者

    Yu, Shin-Shan.;

  • 作者单位

    University of Pennsylvania.;

  • 授予单位 University of Pennsylvania.;
  • 学科 Physics Elementary Particles and High Energy.
  • 学位 Ph.D.
  • 年度 2005
  • 页码 225 p.
  • 总页数 225
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 高能物理学;
  • 关键词

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