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在质子-质子碰撞中寻找轻子+喷注末态下重粒子对产生并衰变为一个顶夸克和一个胶子的过程。 (你提供的原文中“at.”后面缺少具体信息,翻译时根据完整语境补充了合理内容以使句子通顺。)

Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton-proton collisions at .

出版信息

Eur Phys J C Part Fields. 2025;85(3):342. doi: 10.1140/epjc/s10052-024-13729-y. Epub 2025 Mar 25.

DOI:10.1140/epjc/s10052-024-13729-y
PMID:40152191
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11937096/
Abstract

A search is presented for the pair production of new heavy resonances, each decaying into a top quark (t) or antiquark and a gluon (g). The analysis uses data recorded with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 at the LHC, corresponding to an integrated luminosity of 138 . Events with one muon or electron, multiple jets, and missing transverse momentum are selected. After using a deep neural network to enrich the data sample with signal-like events, distributions in the scalar sum of the transverse momenta of all reconstructed objects are analyzed in the search for a signal. No significant deviations from the standard model prediction are found. Upper limits at 95% confidence level are set on the product of cross section and branching fraction squared for the pair production of excited top quarks in the decay channel. The upper limits range from 120 to 0.8 for a with spin-1/2 and from 15 to 1.0 for a with spin-3/2. These correspond to mass exclusion limits up to 1050 and 1700 for spin-1/2 and spin-3/2 particles, respectively. These are the most stringent limits to date on the existence of resonances.

摘要

本文给出了对新的重共振态对产生的搜索,每个共振态衰变成一个顶夸克(t)或反夸克以及一个胶子(g)。该分析使用了CMS探测器在大型强子对撞机(LHC)质心能量为13 TeV时记录的质子 - 质子碰撞数据,对应积分亮度为138 fb⁻¹。选择具有一个μ子或电子、多个喷注以及横向缺失动量的事件。在使用深度神经网络用类信号事件丰富数据样本后,分析所有重建对象横向动量标量和的分布以寻找信号。未发现与标准模型预测有显著偏差。在衰变通道中,对激发顶夸克对产生的截面与分支比平方的乘积设定了95%置信水平的上限。对于自旋为1/2的激发态,上限范围从120到0.8 fb;对于自旋为3/2的激发态,上限范围从15到1.0 fb。这些分别对应自旋为1/2和自旋为3/2粒子质量排除极限高达1050 GeV和1700 GeV。这些是迄今为止对共振态存在最严格的限制。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/9514bf877b45/10052_2024_13729_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/aa55adfd6b32/10052_2024_13729_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/b1ae8d77c944/10052_2024_13729_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/cf67fba0aac7/10052_2024_13729_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/5b69bcf1fe9c/10052_2024_13729_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/13600d5dee2b/10052_2024_13729_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/03bc85365095/10052_2024_13729_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/735adce02ca0/10052_2024_13729_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/9514bf877b45/10052_2024_13729_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/aa55adfd6b32/10052_2024_13729_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/b1ae8d77c944/10052_2024_13729_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/cf67fba0aac7/10052_2024_13729_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/5b69bcf1fe9c/10052_2024_13729_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/13600d5dee2b/10052_2024_13729_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/03bc85365095/10052_2024_13729_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/735adce02ca0/10052_2024_13729_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a13d/11937096/9514bf877b45/10052_2024_13729_Fig8_HTML.jpg

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