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[论文解读] Search for heavy resonances decaying into two Higgs bosons in the $\mathrm{b\bar{b}}τ^+τ^-$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV

CMS Collaboration|arXiv (Cornell University)|Jan 27, 2026
Particle physics theoretical and experimental studies被引用 0
一句话总结

CMS 以 13 TeV 数据(2016–2018,138 fb^-1)搜索重型窄宽度共振体衰变为 Higgs 对(HH),在 bbbar tau tau 最终态下,对质量 1–4.5 TeV 设置 σ(X→HH) 的 95% 置信水平上限。

ABSTRACT

A search is presented for massive narrow-width resonances in the mass range of 1$-$4.5 TeV, decaying into pairs of Higgs bosons (HH). The search uses proton-proton collision data at a center-of-mass energy of 13 TeV collected with the CMS detector at the CERN LHC during 2016$-$2018, corresponding to an integrated luminosity of 138 fb$^{-1}$. The analysis targets final states where one Higgs boson decays into a pair of bottom quarks and the other into a pair of tau leptons, X $ o$ HH $ o$ $\mathrm{b\bar{b}}τ^+τ^-$. It uses a single large jet to reconstruct the H $ o$ $\mathrm{b\bar{b}}$ decay, while the H $ o$ $τ^+τ^-$ decay products can either be contained within a single large jet or appear as two isolated tau leptons. The observed data are consistent with standard model background expectations. Upper limits at 95% confidence level are set on the production cross section for resonant HH production for masses between 1 and 4.5 TeV. This analysis sets the most sensitive limits to date on X $ o$ HH $ o$ $\mathrm{b\bar{b}}τ^+τ^-$ decays in the mass range of 1.4 to 4.5 TeV.

研究动机与目标

  • 推动对衰变为 Higgs 对(HH)的重型共振的超标准模型(BSM)搜索。
  • 在 bbbar τ+τ− 最终态中,通过被强化的 HH 重建,探测共振 HH 产生。
  • 在 1–4.5 TeV 质量范围内,提供自旋-0(辐射子 radion)和自旋-2(引力子 graviton)情景的模型无关敏感性。

提出的方法

  • 使用一套同时适用于自旋-0 与自旋-2 共振衰变为 HH 的分析策略。
  • 通过单个大 jets 重建 H→bb̄ 的一端和另一端 H→τ+τ−(τℓτh 或 τhτh)采用增强型与标准 τ 重建来重建 HH。
  • 用 ParticleNet 对 AK8 jets 的标记来识别 H→bb̄ 候选,并用 DeepJet 在 AK4 jets 上进行 b-标签。
  • 用 FastMTT 与共线近似重建二τ 系统;在 M_HH 标记中进行预选择并定义信号区与边带区。
  • 通过数据驱动和仿真方法估计主导背景(tt̄+jets、W/Z+jets、QCD);使用 Combine 对 M_X 进行分箱最大似然拟合。
Figure 1: A representative diagram for the production of a spin-0 radion or a spin-2 graviton \PX , which decays into two SM Higgs bosons. One Higgs boson decays into a \bbbar pair and the other into a $\PGtp\PGtm$ pair.
Figure 1: A representative diagram for the production of a spin-0 radion or a spin-2 graviton \PX , which decays into two SM Higgs bosons. One Higgs boson decays into a \bbbar pair and the other into a $\PGtp\PGtm$ pair.

实验结果

研究问题

  • RQ1在 1–4.5 TeV 质量范围内,对 resonant HH→bb̄τ+τ− 的产生横截面上限是多少?
  • RQ2是否可以在 bb̄τ+τ− 最终态中用单一分析策略区分或约束自旋-0 与自旋-2 的共振?
  • RQ3增强型 τ 重建和 ParticleNet bb̄ 标记如何提高 boosted HH 区域的灵敏度?

主要发现

  • 对质量在 1 至 4.5 TeV 之间的 σ(X→HH) 设置了 95% CL 上限。
  • 该分析在 1.4–4.5 TeV 范围内对 X→HH→bb̄τ+τ− 的截至目前最敏感的限制。
  • 信号效率在 2–13.5%(τhτh)和 4–11%(ℓτh);背景在全选后以 tt̄+jets 为主导。
  • 背景通过 SB 数据来约束,以归一化并调优 SR 与 SB 中的顶夸克分量的形状。
  • 对 M_X 分布的显式拟合用于提取潜在的共振信号。
Figure 2: Distribution of the invariant mass of the di- \PGt system, reconstructed with the FastMTT algorithm, after the full event selection in the $\tauh\tauh$ (left) and $\Pell\tauh$ (right) channels. The data (solid circles) are compared to the background simulation (filled histograms), where th
Figure 2: Distribution of the invariant mass of the di- \PGt system, reconstructed with the FastMTT algorithm, after the full event selection in the $\tauh\tauh$ (left) and $\Pell\tauh$ (right) channels. The data (solid circles) are compared to the background simulation (filled histograms), where th

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