大型强子对撞机上的极化 $W^+W^-$ 对:NLO QCD+EW 中底夸克诱导过程的影响

Thi Nhung Dao, Duc Ninh Le
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引用次数: 0

摘要

我们研究了底夸克诱导过程对大型强子对撞机上$W^+W^-$成对产生的双极化截面的影响。我们提供了提取壳上单顶贡献的方法。我们给出了在次领先阶(NLO)QCD+EW精度下的现象学和实验分析结果,其中包括了来自胶子-胶子和光子-光子融合的领先贡献。我们发现,在减去壳上$tW$通道之后,底夸克诱导过程的贡献在双纵向极化中是最大的,在有和没有射流否决的两种切割设置中,分别达到了$9\%$和$13\%$的水平(与光夸克贡献的NLO值相比,为综合截面)。计算了各种运动学分布的 $tW$ 干涉约束,结果表明这种干涉效应在无射流否决的情况下一般较小。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Polarized $W^+W^-$ pairs at the LHC: Effects from bottom-quark induced processes at NLO QCD+EW
We investigate the effects of the bottom-quark induced processes on the doubly polarized cross sections of $W^+W^-$ pair production at the LHC. The method to extract the on-shell single-top contribution is provided. Results for phenomenological and experimental analyses are given at next-to-leading order (NLO) QCD+EW accuracy, with the leading contribution from the gluon-gluon and photon-photon fusion included. We found that the contribution of the bottom-quark induced processes, after the subtraction of the on-shell $tW$ channel, is largest for the doubly longitudinal polarization, being at the level of $9\%$ and $13\%$ (compared to the NLO value of the light-quark contribution, for integrated cross section) for two cut setups, with and without a jet veto, respectively. A bound of the $tW$ interference is calculated for various kinematic distributions, showing that this interference effect is, in general, smaller for the no jet veto case.
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