在大型强子对撞机上,味道变化的顶部衰变吸引了一个具有ττ的希格斯玻色子

P. Gutierrez, R. Jain, C. Kao
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引用次数: 1

摘要

我们研究了在欧洲核子研究中心大型强子对撞机(LHC)上发现顶夸克衰变为粲夸克和希格斯玻色子($t \to c h^0$)的前景。采用一般的双希格斯双重态模型来研究变味中性希格斯相互作用。我们使用\textsc{Pythia} 8和\textsc{Delphes}进行了部子级分析和蒙特卡罗模拟,研究了口味变化的顶夸克衰变$t \to c h^0$,随后希格斯衰变为$\tau^+ \tau^-$,另一个顶夸克衰变为一个底夸克($b$)和两个光射流($t\to bW\to bjj$)。为了减少希格斯信号的物理背景,只使用了tau轻子的轻子衰变,$\tau^+\tau^- \to e^\pm\mu^\mp +\slashed{E}_T$,其中$\slashed{E}_T$代表中微子丢失的横向能量。为了重建希格斯玻色子和顶夸克质量,并有效地去除物理背景,采用了高度增强的tau衰变的共线近似。我们的分析表明,$\sqrt{s} = 27$ TeV的高能大型强子对撞机将能够发现具有积分光度$\mathcal{L} = 3$ ab $^{-1}$的FCNH信号,其分支分数${\cal B}(t \to ch^0) \agt 1.4 \times 10^{-4}$对应于FCNH耦合$|\lambda_{tch}| \agt 0.023$。这种FCNH耦合明显低于当前ATLAS组合上限$|\lambda_{tch}| = 0.064$。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flavor changing top decays to charm and a Higgs boson with ττ at the LHC
We investigate the prospects of discovering the top quark decay into a charm quark and a Higgs boson ($t \to c h^0$) in top quark pair production at the CERN Large Hadron Collider (LHC). A general two Higgs doublet model is adopted to study flavor changing neutral Higgs (FCNH) interactions. We perform a parton level analysis as well as Monte Carlo simulations using \textsc{Pythia}~8 and \textsc{Delphes} to study the flavor changing top quark decay $t \to c h^0$, followed by the Higgs decaying into $\tau^+ \tau^-$, with the other top quark decaying to a bottom quark ($b$) and two light jets ($t\to bW\to bjj$). To reduce the physics background to the Higgs signal, only the leptonic decays of tau leptons are used, $\tau^+\tau^- \to e^\pm\mu^\mp +\slashed{E}_T$, where $\slashed{E}_T$ represents the missing transverse energy from the neutrinos. In order to reconstruct the Higgs boson and top quark masses as well as to effectively remove the physics background, the collinear approximation for the highly boosted tau decays is employed. Our analysis suggests that a high energy LHC at $\sqrt{s} = 27$ TeV will be able to discover this FCNH signal with an integrated luminosity $\mathcal{L} = 3$ ab$^{-1}$ for a branching fraction ${\cal B}(t \to ch^0) \agt 1.4 \times 10^{-4}$ that corresponds to a FCNH coupling $|\lambda_{tch}| \agt 0.023$. This FCNH coupling is significantly below the current ATLAS combined upper limit of $|\lambda_{tch}| = 0.064$.
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