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arXiv 2407.03501hep-ph
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顶-反顶强子产生中 NNLL+NNLO 的 $q_{\mathrm{T}}$ 与 $Δϕ_{t\bar{t}}$ 谱:软-共线重求和与库仑奇点的相互作用

The $q_{\mathrm{T}}$ and $Δϕ_{t\bar{t}}$ spectra in top-antitop hadroproduction at NNLL+NNLO: the interplay of soft-collinear resummation and Coulomb singularities

Wan-Li Ju, Marek Schoenherr

AI总结:

本文在 NNLL+NNLO 精度下计算 LHC 顶夸克对产生的横动量谱和方位角退关联谱,提出 D-处方和 R-处方处理阈值区域的库仑奇点,并定量评估了处方选择带来的理论不确定性。

摘要:

本文给出了 LHC 上顶-反顶对产生中经重求和改进的微分横动量谱和方位角退关联截面 $dσ_{t\bar{t}}/dq_{\mathrm{T}}$ 与 $dσ_{t\bar{t}}/dΔϕ_{t\bar{t}}$。我们的计算基于如下观察:在 $\sqrt{s}=13\\,\text{TeV}$ 或更高的对撞能量下,这两个截面都由顶夸克对良好分离的拓扑主导,其相对速度 $β_{t\bar{t}}\sim\mathcal{O}(1)$。因此,$q_{\mathrm{T}}\to0$ 和 $Δϕ_{t\bar{t}}\to0$ 极限下的渐近行为主要可由 HQET$+$SCET 框架中的软与共线重求和来刻画。然而,从 NNLL 开始,在阈值区域 $β_{t\bar{t}}\to0$ 中,硬部分及其演化核都会出现库仑奇点,导致对整个 $β_{t\bar{t}}$ 范围积分时得到非物理结果。为此,我们引入了两种处方,称为 D-处方和 R-处方,来正规化这些库仑奇点。它们体现了两种截断阈值增强项的根本不同方法,使其贡献有限。在缺乏阈值与小横动量联合重求和的情况下,我们对两种 $dσ_{t\bar{t}}/dq_{\mathrm{T}}$ 和 $dσ_{t\bar{t}}/dΔϕ_{t\bar{t}}$ 谱分别给出了由处方选择所引入的模糊性的定量评估,这本身也检验了我们的计算对此类阈值增强的敏感度。

英文摘要:

In this paper, we present the resummation-improved differential transverse momentum and azimuthal decorrelation cross sections, $dσ_{t\bar{t}}/dq_{\mathrm{T}}$ and $dσ_{t\bar{t}}/dΔϕ_{t\bar{t}}$, in top-antitop pair production at the LHC. Our calculation is based on the observation that both cross sections are dominated by topologies where the top-quark pair is well separated, expressed in their relative velocity $β_{t\bar{t}}\sim\mathcal{O}(1)$, at colliding energies of $\sqrt{s}=13\,\text{TeV}$ or higher. Therefore, the asymptotic behaviour in the limits $q_{\mathrm{T}}\to0$ and $Δϕ_{t\bar{t}}\to0$ can mostly be captured by the soft and collinear resummation in the HQET$+$SCET framework. Nevertheless, starting at NNLL, Coulomb singularities emerge in the threshold regime, $β_{t\bar{t}}\to0$, in both the hard sector and its evolution kernels, leading to unphysical results upon integration over the entire $β_{t\bar{t}}$ range. To this end, two prescriptions, dubbed the D- and R-prescription, are introduced to regularise these Coulomb singularities. They embody two fundamentally different methods to truncate the threshold enhanced terms, rendering their contribution finite. In the absence of a combined threshold and small-transverse-momentum resummation, we present a quantitative assessment of the ambiguity introduced by the choice of prescription, itself a test of the sensitivity of our calculation to such threshold enhancements, for both the $dσ_{t\bar{t}}/dq_{\mathrm{T}}$ and $dσ_{t\bar{t}}/dΔϕ_{t\bar{t}}$ spectra.

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