Synthesis on Heavy Higgs from the Standard Model to 2HDM and Beyond

Abdeljalil Habjia
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Abstract

In the context of particle physics, within the ATLAS and CMS experiments at large hadron collider (LHC), this work presents the discussion of the discovery of a particle compatible with the Higgs boson by the combination of several decay channels, with a mass of the order of 125.5 GeV. With increased statistics, that is the full set of data collected by the ATLAS and CMS experiments at LHC ( s1/2 = 7GeV and s1/2 = 8GeV ), the particle is also discovered individually in the channel h-->γγ with an observed significance of 5.2σ and 4.7σ, respectively. The analysis dedicated to the measurement of the mass mh and signal strength μ which is defined as the ratio of σ(pp --> h) X Br(h-->X) normalized to its Standard Model where X = WW*; ZZ*; γγ ; gg; ff. The combined results in h-->γγ channel gave the measurements: mh = 125:36 ± 0:37Gev, (μ = 1:17 ± 0:3) and the constraint on the width Γ(h) of the Higgs decay of 4.07 MeV at 95%CL. The spin study rejects the hypothesis of spin 2 at 99 %CL. The odd parity (spin parity 0- state) is excluded at more than 98%CL. Within the theoretical and experimental uncertainties accessible at the time of the analysis, all results: channels showing the excess with respect to the background-only hypothesis, measured mass and signal strength, couplings, quantum numbers (JPC), production modes, total and differential cross-sections, are compatible with the Standard Model Higgs boson at 95%CL. Although the Standard Model is one of the theories that have experienced the greatest number of successes to date, it is imperfect. The inability of this model to describe certain phenomena seems to suggest that it is only an approximation of a more general theory. Models beyond the Standard Model, such as 2HDM, MSSM or NMSSM, can compensate some of its limitations and postulate the existence of additional Higgs bosons.
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从标准模型到2HDM及更高的重希格斯粒子的综合
在粒子物理学的背景下,在大型强子对撞机(LHC)的ATLAS和CMS实验中,本文讨论了通过几个衰变通道的组合发现与希格斯玻色子兼容的粒子,其质量为125.5 GeV。随着统计量的增加,即LHC上ATLAS和CMS实验收集的全套数据(s1/2 = 7GeV和s1/2 = 8GeV),在h- >γγ通道中也单独发现了该粒子,观测到的显著性分别为5.2σ和4.7σ。该分析专门用于测量质量mh和信号强度μ,其定义为σ(pp -> h) X Br(h- >X)归一化到其标准模型的比率,其中X = WW*;ZZ *;γγ;gg;ff。h- > Γ Γ通道的综合结果得到:mh = 125:36±0:37Gev, (μ = 1:17±0:3)和95%CL下4.07 MeV的希格斯衰变宽度Γ(h)约束。自旋研究拒绝了自旋2在99% CL下的假设。奇宇称(自旋宇称0-态)在超过98%CL时被排除。在分析时可获得的理论和实验不确定度范围内,所有结果:显示相对于纯背景假设、测量质量和信号强度、耦合、量子数(JPC)、产生模式、总横截面和微分横截面的通道,在95%CL下与标准模型希格斯玻色子兼容。尽管标准模型是迄今为止获得最多成功的理论之一,但它并不完美。这个模型无法描述某些现象,似乎表明它只是一个更一般理论的近似值。超出标准模型的模型,如2HDM、MSSM或NMSSM,可以弥补它的一些局限性,并假设存在额外的希格斯玻色子。
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