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Application of the Principle of Maximum Conformality to the Top-Quark Charge Asymmetry at the LHC

机译:最大共形原理在顶夸克中的应用   在LHC充电不对称

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摘要

The Principle of Maximum Conformality (PMC) provides a systematic andprocess-independent method to derive renormalization scheme- and scale-independent fixed-order pQCD predictions. In Ref.\cite{pmc3}, we studied thetop-quark charge asymmetry at the Tevatron. By applying the PMC, we have shownthat the large discrepancies for the top-quark charge asymmetry between theStandard Model estimate and the CDF and D0 data are greatly reduced. In thepresent paper, with the help of the Bernreuther-Si program, we present adetailed PMC analysis on the top-quark pair production up tonext-to-next-to-leading order level at the LHC. After applying PMC scalesetting, the pQCD prediction for the top-quark charge asymmetry at the LHC hasvery small scale uncertainty; e.g., $A_{\rm C}|_{\rm 7 TeV;PMC}=\left(1.15^{+0.01}_{-0.03}\right)\%$, $A_{\rm C}|_{\rm 8 TeV;PMC}=\left(1.03^{+0.01}_{+0.00}\right)\%$, and $A_{\rm C}|_{\rm 14 TeV;PMC}=\left(0.62^{+0.00}_{-0.02}\right)\%$. The corresponding predictions usingconventional scale setting are: $A_{\rm C}|_{\rm 7 TeV;Conv.}=\left(1.23^{+0.14}_{-0.14}\right)\%$, $A_{\rm C}|_{\rm 8 TeV;Conv.}=\left(1.11^{+0.17}_{-0.13}\right)\%$, and $A_{\rm C}|_{\rm 14 TeV;Conv.}=\left(0.67^{+0.05}_{-0.05}\right)\%$. In these predictions, the scale errorsare predicted by varying the initial renormalization and factorization scalesin the ranges $\mu^{\rm init}_r\in[m_t/2,2m_t]$ and $\mu_f\in[m_t/2,2m_t]$. ThePMC predictions are also in better agreement with the available ATLAS and CMSdata. In addition, we have calculated the top-quark charge asymmetry assumingseveral typical cuts on the top-pair invariant mass $M_{t\bar{t}}$. Forexample, assuming $M_{t\bar{t}}>0.5 ~ {\rm TeV}$ and $\mu_f=\mu^{\rm init}_r=m_t$, we obtain $A_{\rm C}|_{\rm 7 TeV;PMC}=2.67\%$, $A_{\rm C}|_{\rm 8TeV;PMC}=2.39\%$, and $A_{\rm C}|_{\rm 14 TeV;PMC}=1.28\%$.
机译:最大适形性原理(PMC)提供了一种系统的,与过程无关的方法来推导重归一化方案和与比例无关的固定阶pQCD预测。在Ref。\ cite {pmc3}中,我们研究了Tevatron的顶夸克电荷不对称性。通过应用PMC,我们已经证明,标准模型估计值与CDF和D0数据之间的最大夸克电荷不对称性差异大大减小。在本文中,借助Bernreuther-Si计划,我们对大型强子对撞机从头到尾到头到尾的顶级夸克对生产进行了详细的PMC分析。在应用PMC标定之后,大型强子对撞机顶夸克电荷不对称的pQCD预测具有很小的标度不确定性;例如,$ A _ {\ rm C} | _ {\ rm 7 TeV; PMC} = \ left(1.15 ^ {+ 0.01} _ {-0.03} \ right)\%$,$ A _ {\ rm C} | _ {\ rm 8 TeV; PMC} = \左(1.03 ^ {+ 0.01} _ {+ 0.00} \ right)\%$和$ A _ {\ rm C} | _ {\ rm 14 TeV; PMC} = \左(0.62 ^ {+ 0.00} _ {-0.02} \右)\%$。使用常规比例尺设置的相应预测为:$ A _ {\ rm C} | _ {\ rm 7 TeV; Conv。} = \ left(1.23 ^ {+ 0.14} _ {-0.14} \ right)\%$,$ A_ {\ rm C} | _ {\ rm 8 TeV; Conv。} = \ left(1.11 ^ {+ 0.17} _ {-0.13} \ right)\%$和$ A _ {\ rm C} | _ {\ rm 14 TeV; Conv。} = \ left(0.67 ^ {+ 0.05} _ {-0.05} \ right)\%$。在这些预测中,通过在$ \ mu ^ {\ rm init} _r \ in [m_t / 2,2m_t] $和$ \ mu_f \ in [m_t / 2,2m_t ] $。 PMC的预测也与可用的ATLAS和CMSdata更好地吻合。此外,我们假设顶对不变质量$ M_ {t \ bar {t}} $有几个典型削减,因此我们计算了顶夸克电荷不对称性。例如,假设$ M_ {t \ bar {t}}> 0.5〜{\ rm TeV} $和$ \ mu_f = \ mu ^ {\ rm init} _r = m_t $,我们得到$ A _ {\ rm C} | _ {\ rm 7 TeV; PMC} = 2.67 \%$,$ A _ {\ rm C} | _ {\ rm 8TeV; PMC} = 2.39 \%$和$ A _ {\ rm C} | _ {\ rm 14 TeV; PMC} = 1.28 \%$。

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