Single and Pair Production of Excited Top Quarks in Hadronic Collisions at \({\sqrt{s}=13}\) and \({14}\) TeV

IF 0.5 4区 物理与天体物理 Q4 PHYSICS, NUCLEAR
Eduard Boos, Viacheslav Bunichev, Sergei Trykov, Guliya Nurbakova, Saniya Rustembayeva
{"title":"Single and Pair Production of Excited Top Quarks in Hadronic Collisions at \\({\\sqrt{s}=13}\\) and \\({14}\\) TeV","authors":"Eduard Boos,&nbsp;Viacheslav Bunichev,&nbsp;Sergei Trykov,&nbsp;Guliya Nurbakova,&nbsp;Saniya Rustembayeva","doi":"10.1134/S106377882660020X","DOIUrl":null,"url":null,"abstract":"<p>We explore the collider phenomenology of spin-<span>\\(1/2\\)</span> excited top quarks arising from QCD-invariant magnetic transition operators, motivated by scenarios in which Standard Model fermions are composite objects. Assuming the absence of electroweak and contact interactions, we consider a minimal effective field theory framework where the excited top decays exclusively via the strong channel <span>\\(t^{*}\\to tg\\)</span>. Both pair and single excited top production are studied at proton–proton colliders with center-of-mass energies <span>\\(\\sqrt{s}=13\\)</span> and <span>\\(14\\)</span> TeV, corresponding to the LHC and HL-LHC regimes. We compute the total cross sections for both production modes, including all gauge and magnetic contributions, and examine their dependence on the compositeness scale <span>\\(\\Lambda\\)</span> and excited top mass <span>\\(m_{t^{*}}\\)</span>. While pair production proceeds primarily through minimal QCD couplings and exhibits limited sensitivity to <span>\\(\\Lambda\\)</span>, single production is governed by the magnetic transition operator and provides a complementary probe with distinct kinematic features. Our results highlight the dominant role of single production across a wide region of parameter space, particularly in the natural scenario <span>\\(\\Lambda=m_{t^{*}}\\)</span>, underscoring its relevance for future searches targeting excited top signatures with boosted topologies.</p>","PeriodicalId":728,"journal":{"name":"Physics of Atomic Nuclei","volume":"89 1","pages":"62 - 68"},"PeriodicalIF":0.5000,"publicationDate":"2026-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physics of Atomic Nuclei","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1134/S106377882660020X","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
引用次数: 0

Abstract

We explore the collider phenomenology of spin-\(1/2\) excited top quarks arising from QCD-invariant magnetic transition operators, motivated by scenarios in which Standard Model fermions are composite objects. Assuming the absence of electroweak and contact interactions, we consider a minimal effective field theory framework where the excited top decays exclusively via the strong channel \(t^{*}\to tg\). Both pair and single excited top production are studied at proton–proton colliders with center-of-mass energies \(\sqrt{s}=13\) and \(14\) TeV, corresponding to the LHC and HL-LHC regimes. We compute the total cross sections for both production modes, including all gauge and magnetic contributions, and examine their dependence on the compositeness scale \(\Lambda\) and excited top mass \(m_{t^{*}}\). While pair production proceeds primarily through minimal QCD couplings and exhibits limited sensitivity to \(\Lambda\), single production is governed by the magnetic transition operator and provides a complementary probe with distinct kinematic features. Our results highlight the dominant role of single production across a wide region of parameter space, particularly in the natural scenario \(\Lambda=m_{t^{*}}\), underscoring its relevance for future searches targeting excited top signatures with boosted topologies.

Abstract Image

\({\sqrt{s}=13}\)和\({14}\) TeV强子碰撞中激发顶夸克的单对产生
在标准模型费米子是复合物体的情况下,我们探索了由qcd不变磁跃迁算子产生的自旋\(1/2\)激发顶夸克的对撞机现象学。假设没有电弱相互作用和接触相互作用,我们考虑了一个最小有效场论框架,其中激发顶只通过强通道\(t^{*}\to tg\)衰减。在质心能量分别为\(\sqrt{s}=13\)和\(14\) TeV的质子-质子对撞机上,分别研究了LHC和HL-LHC体制下的对激和单激顶产生。我们计算了两种生产模式的总横截面,包括所有规范和磁贡献,并检查了它们对复合尺度\(\Lambda\)和受激顶质量\(m_{t^{*}}\)的依赖。虽然对生产主要通过最小的QCD耦合进行,并且对\(\Lambda\)的灵敏度有限,但单生产由磁过渡算子控制,并提供具有独特运动学特征的互补探头。我们的研究结果强调了单次生成在广泛的参数空间区域中的主导作用,特别是在自然场景\(\Lambda=m_{t^{*}}\)中,强调了其与未来搜索的相关性,这些搜索目标是具有增强拓扑的激发顶级签名。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
Physics of Atomic Nuclei
Physics of Atomic Nuclei 物理-物理:核物理
CiteScore
0.60
自引率
25.00%
发文量
56
审稿时长
3-6 weeks
期刊介绍: Physics of Atomic Nuclei is a journal that covers experimental and theoretical studies of nuclear physics: nuclear structure, spectra, and properties; radiation, fission, and nuclear reactions induced by photons, leptons, hadrons, and nuclei; fundamental interactions and symmetries; hadrons (with light, strange, charm, and bottom quarks); particle collisions at high and superhigh energies; gauge and unified quantum field theories, quark models, supersymmetry and supergravity, astrophysics and cosmology.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信
小红书