{"title":"Sharpening the A → Z(*)h signature of the Type-II 2HDM at the LHC through advanced Machine Learning","authors":"W. Esmail, A. Hammad, S. Moretti","doi":"10.1007/jhep11(2023)020","DOIUrl":null,"url":null,"abstract":"A bstract The A → Z (*) h decay signature has been highlighted as possibly being the first testable probe of the Standard Model (SM) Higgs boson discovered in 2012 ( h ) interacting with Higgs companion states, such as those existing in a 2-Higgs Doublet Model (2HDM), chiefly, a CP-odd one ( A ). The production mechanism of the latter at the Large Hadron Collider (LHC) takes place via $$ b\\overline{b} $$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mi>b</mml:mi> <mml:mover> <mml:mi>b</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> -annihilation and/or gg -fusion, depending on the 2HDM parameters, in turn dictated by the Yukawa structure of this Beyond the SM (BSM) scenario. Among the possible incarnations of the 2HDM, we test here the so-called Type-II, for a twofold reason. On the one hand, it intriguingly offers two very distinct parameter regions compliant with the SM-like Higgs measurements, i.e., where the so-called ‘SM limit’ of the 2HDM can be achieved. On the other hand, in both configurations, the AZh coupling is generally small, hence the signal is strongly polluted by backgrounds, so that the exploitation of Machine Learning (ML) techniques becomes extremely useful. In this paper, we show that the application of advanced ML implementations can be decisive in establishing such a signal. This is true for all distinctive kinematical configurations involving the A → Z (*) h decay, i.e., below threshold ( m A < m Z + m h ), at its maximum ( m Z + m h < m A < 2 m t ) and near the onset of $$ t\\overline{t} $$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> pair production ( m A ≈ 2 m t ), for which we propose Benchmark Points (BPs) for future phenomenological analyses.","PeriodicalId":48906,"journal":{"name":"Journal of High Energy Physics","volume":"12 6","pages":"0"},"PeriodicalIF":5.0000,"publicationDate":"2023-11-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of High Energy Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1007/jhep11(2023)020","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
引用次数: 0
Abstract
A bstract The A → Z (*) h decay signature has been highlighted as possibly being the first testable probe of the Standard Model (SM) Higgs boson discovered in 2012 ( h ) interacting with Higgs companion states, such as those existing in a 2-Higgs Doublet Model (2HDM), chiefly, a CP-odd one ( A ). The production mechanism of the latter at the Large Hadron Collider (LHC) takes place via $$ b\overline{b} $$ bb¯ -annihilation and/or gg -fusion, depending on the 2HDM parameters, in turn dictated by the Yukawa structure of this Beyond the SM (BSM) scenario. Among the possible incarnations of the 2HDM, we test here the so-called Type-II, for a twofold reason. On the one hand, it intriguingly offers two very distinct parameter regions compliant with the SM-like Higgs measurements, i.e., where the so-called ‘SM limit’ of the 2HDM can be achieved. On the other hand, in both configurations, the AZh coupling is generally small, hence the signal is strongly polluted by backgrounds, so that the exploitation of Machine Learning (ML) techniques becomes extremely useful. In this paper, we show that the application of advanced ML implementations can be decisive in establishing such a signal. This is true for all distinctive kinematical configurations involving the A → Z (*) h decay, i.e., below threshold ( m A < m Z + m h ), at its maximum ( m Z + m h < m A < 2 m t ) and near the onset of $$ t\overline{t} $$ tt¯ pair production ( m A ≈ 2 m t ), for which we propose Benchmark Points (BPs) for future phenomenological analyses.
A→Z (*) h衰变特征被强调为可能是2012年发现的标准模型(SM)希格斯玻色子(h)与希格斯伴生态相互作用的第一个可测试探测,例如存在于2-希格斯双重态模型(2HDM)中的那些,主要是一个cp奇数(A)。后者在大型强子对撞机(LHC)上的产生机制是通过$$ b\overline{b} $$ b¯湮灭和/或gg -聚变发生的,这取决于2HDM参数,而这又取决于这个超越SM (BSM)场景的汤川结构。在可能的2HDM版本中,我们在这里测试所谓的Type-II,有两个原因。一方面,有趣的是,它提供了两个非常不同的参数区域,符合类标准希格斯测量,即,所谓的2HDM的“标准SM极限”可以实现。另一方面,在这两种配置中,AZh耦合通常很小,因此信号受到背景的强烈污染,因此机器学习(ML)技术的利用变得非常有用。在本文中,我们证明了高级机器学习实现的应用对于建立这样的信号是决定性的。这对于涉及A→Z (*) h衰减的所有不同的运动学构型都是正确的,即低于阈值(m A &lt;m Z + m h),在其最大值(m Z + m h &lt;m &;2 m t)和接近$$ t\overline{t} $$ t t¯对生产(m A≈2 m t)的开始(m A≈2 m t),我们提出了用于未来现象学分析的基准点(bp)。
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