在\(\sqrt{s}\) = 13,14,27和100 TeV同时产生的希格斯玻色子和矢量玻色子的QCD预测,并综合研究了系统不确定性和电荷不对称性

IF 4.8 2区 物理与天体物理 Q2 PHYSICS, PARTICLES & FIELDS
Kamuran Dilsiz, Emrah Tiras, Meryem Yilmaz, Hasan Ogul
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引用次数: 0

摘要

本文在\(\sqrt{s} = 13, 14, 27\)和100 TeV上对希格斯玻色子同时产生的矢量玻色子的高阶QCD截面进行了全面研究。希格斯粒子与矢量玻色子的同时产生有助于对希格斯信号的研究。在计算中,考虑了希格斯粒子(\(\tau ^{-}\tau ^{+}\), \(b{\bar{b}}\), \(\gamma \gamma \))和矢量玻色子(\(W^{\pm }(e^{\pm }\nu ({\bar{\nu }})), Z(e^{-}e^{+}\))的三种不同分支态。在这里,计算了这些分支状态的前导阶(LO)、次导阶(NLO)和次导阶(NNLO) QCD截面。在TRUBA高性能网格计算中心建立了仿真框架。然后,选择与CMS和ATLAS合作使用的值接近的阈值(选择切割),并将其用于恒定质量、横向动量(\(p_{T}\))、伪快度(\(\eta \))等参数。计算时采用NNPDF3.1部分分布函数(parton distribution functions, PDF)。结果表明,NLO和NNLO的QCD预测值均比LO预测值高。除了高阶外,截面值随质心能量的增加而增加。除QCD预测外,还计算了QCD预测的PDF、规模和\(\alpha _{S}\)不确定性,以检验高阶QCD的可靠性。结果表明,随着QCD阶数的增加,总不确定性和尺度不确定性减小。此外,随着质心能量的增加,LO的总不确定性和尺度不确定性显著增加,而NLO和NNLO的尺度和总不确定性随着质心能量的增加几乎保持不变或增加可以忽略不计。这表明高阶量子cds不仅通过增加额外的部分子图提供了更准确的结果,而且在相关的生产通道中提供了更低的不确定性。此外,为同时产生的希格斯玻色子和矢量玻色子的物理测量提供精确统计所需的数据,如13tev的数据,预测为\(\sqrt{s}\) = 14,27和100tev。结果,我们发现,在\(\sqrt{s}\) = 14、27和100 TeV下,数据量分别比\(\sqrt{s}\) = 13 TeV下少1.1倍、2.0倍和6.5倍,可以获得相同的精确物理测量统计数据。在本研究的最后一部分,在NNLO QCD上计算了W玻色子的电荷不对称性。在WH(\(\tau ^{-}\tau ^{+}\))衰变通道获得了\(W^{+}\)和\(W^{-}\)之间最低的电荷不对称,在WH(\(b{\bar{b}}\))衰变通道获得了最高的电荷不对称结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
QCD predictions for simultaneously produced Higgs and vector bosons at \(\sqrt{s}\) = 13, 14, 27 and 100 TeV with a comprehensive study of systematic uncertainty and charge asymmetry

A comprehensive study of high-order QCD cross-section for the Higgs boson that is simultaneously produced with a vector boson is presented at \(\sqrt{s} = 13, 14, 27\) and 100 TeV in this manuscript. The simultaneous Higgs production with a vector boson facilitates the investigation of the Higgs signal. In the calculations, three different branching states of the Higgs (\(\tau ^{-}\tau ^{+}\), \(b{\bar{b}}\), \(\gamma \gamma \)) and vector bosons [\(W^{\pm }(e^{\pm }\nu ({\bar{\nu }})), Z(e^{-}e^{+}\))] were taken into account. Here, leading order (LO), next-to-leading order (NLO), and next-to-NLO (NNLO) QCD cross-sections were calculated for these branching states. A simulation framework was built for the calculations at the TRUBA high-performance grid computing center. Then, the threshold values (selection cuts) close to the values used by the CMS and ATLAS Collaborations were selected and used on several parameters such as invariant mass, transverse momentum (\(p_{T}\)), pseudorapidity (\(\eta \)), etc. In addition, NNPDF3.1 parton distribution functions (PDF) were used during the calculation. The results showed that the numerical value of the QCD prediction increases at NLO and NNLO as compared to the LO predictions. In addition to the higher-orders, the cross-section value increases as the center-of-mass energy increases. In addition to the QCD predictions, PDF, scale, and \(\alpha _{S}\) uncertainties of the QCD predictions were also calculated to test the reliability of the high-order QCDs. The results showed that total and scale uncertainties decrease as the QCD order increases. In addition, it was found that LO total and scale uncertainties increase significantly as the center-of-mass energy increases, while NLO and NNLO scale and total uncertainties remain almost constant or show a negligible increase as the center-of-mass energy increases. This indicates that high-order QCDs not only provide more accurate results by the addition of extra partonic diagrams but also provide lower uncertainties in the relevant production channels. Furthermore, the required data that provides the exact statistics for physics measurements of simultaneously produced Higgs and vector bosons as the data at 13 TeV were predicted at \(\sqrt{s}\) = 14, 27, and 100 TeV. As a result, we found that the same statistics for accurate physics measurements can be obtained at \(\sqrt{s}\) = 14, 27, and 100 TeV with approximately 1.1, 2.0, and 6.5 times less data than the amount of data at \(\sqrt{s}\) = 13 TeV, respectively. In the last section of this study, W boson charge asymmetry was computed at NNLO QCD. The lowest charge asymmetry between \(W^{+}\) and \(W^{-}\) was obtained at the WH(\(\tau ^{-}\tau ^{+}\)) decay channel and the highest charge asymmetry results were obtained at the WH(\(b{\bar{b}}\)) decay channel.

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来源期刊
The European Physical Journal C
The European Physical Journal C 物理-物理:粒子与场物理
CiteScore
8.10
自引率
15.90%
发文量
1008
审稿时长
2-4 weeks
期刊介绍: Experimental Physics I: Accelerator Based High-Energy Physics Hadron and lepton collider physics Lepton-nucleon scattering High-energy nuclear reactions Standard model precision tests Search for new physics beyond the standard model Heavy flavour physics Neutrino properties Particle detector developments Computational methods and analysis tools Experimental Physics II: Astroparticle Physics Dark matter searches High-energy cosmic rays Double beta decay Long baseline neutrino experiments Neutrino astronomy Axions and other weakly interacting light particles Gravitational waves and observational cosmology Particle detector developments Computational methods and analysis tools Theoretical Physics I: Phenomenology of the Standard Model and Beyond Electroweak interactions Quantum chromo dynamics Heavy quark physics and quark flavour mixing Neutrino physics Phenomenology of astro- and cosmoparticle physics Meson spectroscopy and non-perturbative QCD Low-energy effective field theories Lattice field theory High temperature QCD and heavy ion physics Phenomenology of supersymmetric extensions of the SM Phenomenology of non-supersymmetric extensions of the SM Model building and alternative models of electroweak symmetry breaking Flavour physics beyond the SM Computational algorithms and tools...etc.
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