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强子对撞机上包含W[公式:见原文]产生的标度性质。

Scaling properties of inclusive W[Formula: see text] production at hadron colliders.

作者信息

Arleo François, Chapon Émilien, Paukkunen Hannu

机构信息

Laboratoire Leprince-Ringuet, École polytechnique, CNRS/IN2P3, Université Paris-Saclay, 91128 Palaiseau, France.

Department of Physics, University of Jyvaskyla, P.O. Box 35, 40014 University of Jyvaskyla, Finland.

出版信息

Eur Phys J C Part Fields. 2016;76(4):214. doi: 10.1140/epjc/s10052-016-4049-1. Epub 2016 Apr 18.

DOI:10.1140/epjc/s10052-016-4049-1
PMID:28260975
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5312166/
Abstract

We consider the hadroproduction of W gauge bosons in their leptonic decay mode. Starting from the leading-order expressions, we show that by defining a suitable scaling variable the centre-of-mass dependence of the cross sections at the LHC energies can be essentially described by a simple power law. The scaling exponent is directly linked to the small- behaviour of parton distribution functions (PDF) which, at the high virtualities involved in W production, is largely dictated by QCD evolution equations. This entails a particularly simple scaling law for the lepton charge asymmetry and also predicts that measurements in different collision systems (p-p, p-[Formula: see text], p-Pb Pb-Pb) are straightforwardly related. The expectations are compared with the existing data and a very good overall agreement is observed. It is shown that the PDF uncertainty in certain cross-section ratios between nearby centre-of-mass energies can be significantly reduced by taking the ratios at fixed value of the scaling variable instead of fixed rapidity.

摘要

我们考虑W规范玻色子在轻子衰变模式下的强子产生过程。从领头阶表达式出发,我们表明通过定义一个合适的标度变量,大型强子对撞机(LHC)能量下截面的质心依赖性基本上可以用一个简单的幂律来描述。标度指数直接与部分子分布函数(PDF)的小x行为相关,在W产生所涉及的高虚能情况下,这种行为在很大程度上由量子色动力学(QCD)演化方程决定。这导致了轻子电荷不对称性的一个特别简单的标度律,并且还预测了在不同碰撞系统(质子 - 质子、质子 - 反质子、质子 - 铅离子、铅离子 - 铅离子)中的测量结果是直接相关的。我们将这些预期与现有数据进行了比较,观察到了非常好的总体一致性。结果表明,通过在固定标度变量值而非固定快度下取比值,可以显著降低相邻质心能量之间某些截面比中的PDF不确定性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/9da38a0e403f/10052_2016_4049_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/cc7d257eb8d6/10052_2016_4049_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/09883224f123/10052_2016_4049_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/449b961106eb/10052_2016_4049_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/1386bc0ebd07/10052_2016_4049_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/7ab6fd60ef01/10052_2016_4049_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/59398aa2b764/10052_2016_4049_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/99081c918af8/10052_2016_4049_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/dfa87dcaf338/10052_2016_4049_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/9da38a0e403f/10052_2016_4049_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/cc7d257eb8d6/10052_2016_4049_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/09883224f123/10052_2016_4049_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/449b961106eb/10052_2016_4049_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/1386bc0ebd07/10052_2016_4049_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/7ab6fd60ef01/10052_2016_4049_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/59398aa2b764/10052_2016_4049_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/99081c918af8/10052_2016_4049_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/dfa87dcaf338/10052_2016_4049_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5eda/5312166/9da38a0e403f/10052_2016_4049_Fig9_HTML.jpg

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