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arXiv 2406.07643hep-phhep-ex
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一个17 MeV赝标量与LSND、MiniBooNE和ATOMKI异常

A 17 MeV pseudoscalar and the LSND, MiniBooNE and ATOMKI anomalies

Waleed Abdallah, Raj Gandhi, Tathagata Ghosh, Najimuddin Khan, Samiran Roy, Subhojit Roy

AI总结:

本文提出含17 MeV赝标量媒介子、第二Higgs二重态和三个单态中微子的SM扩展,以联合解释LSND、MiniBooNE及ATOMKI异常,并分析实验约束与未来检验。

摘要:

在大型强子对撞机(LHC)尚未出现任何新物理信号的情况下,低能实验中的异常结果日益受到关注。我们聚焦于来自LSND、MiniBooNE(MB)和ATOMKI实验的三个此类结果。一个17 MeV的赝标量媒介子($a'$)可以解释ATOMKI中成对产生跃迁里观测到超额事件的三种情形中的两种($^8$Be和$^4$He)。我们将该媒介子纳入标准模型(SM)的一个规范不变扩展中,该扩展包含第二个Higgs二重态和三个单态(跷跷板)中微子($N_i, i=1,2,3$)。$N_{1,2}$参与MB和LSND中的一种相互作用;在以$a'$为媒介子时,该相互作用导致$e^+ e^-$对的产生。$N_i$还会产生SM中微子的质量平方差,并与全局振荡数据一致。我们首先表明,这样的模型为MB和LSND超额提供了自然的联合解决方案,并对其数据给出极佳拟合。随后,利用解释ATOMKI中$^8$Be和$^4$He成对产生核跃迁数据所需的夸克和电子耦合取值,我们表明这些取值仍能拟合MB和LSND数据。然而,一旦纳入ATOMKI,来自衰变$K^+ \ ightarrow π^+ a'\,(a'\ ightarrow e^+e^-)$和$π^+ \ ightarrow e^+ ν_e e^+ e^-$的强约束便会发挥作用。尽管我们的解符合前一衰变的界限,但仍与后者的90% CL界限存在张力。我们还讨论了来自对撞机与非对撞机实验以及电弱精确数据、稳定性和幺正性的其他约束。我们计算了模型中直至两圈对电子和μ子$g-2$的贡献,并讨论了该模型在未来实验中的检验。

英文摘要:

In the absence of any new physics signals at the Large Hadron Collider (LHC), anomalous results at low energy experiments have become the subject of increased attention. We focus on three such results from the LSND, MiniBooNE (MB), and ATOMKI experiments. A 17 MeV pseudoscalar mediator ($a'$) can account for two ($^8$Be and $^4$He) out of the three cases in which excess events have been seen in pair creation transitions in ATOMKI. We incorporate this mediator in a gauge invariant extension of the Standard Model (SM) with a second Higgs doublet and three singlet (seesaw) neutrinos ($N_i, i=1,2,3$). $N_{1,2}$ participate in an interaction in MB and LSND which, with $a'$ as mediator, leads to the production of $e^+ e^-$ pairs. The $N_i$ also lead to mass-squared differences for SM neutrinos in agreement with global oscillation data. We first show that such a model offers a natural joint solution to the MB and LSND excesses, providing excellent fits to their data. Next, using the values of the couplings to the quarks and electrons which are required to explain pair creation nuclear transition data for $^8$Be and $^4$He in ATOMKI, we show that these values still lead to fits for MB and LSND data. However, once ATOMKI is incorporated, we find that strong constraints from the decays $K^+ \rightarrow π^+ a' \, (a'\rightarrow e^+e^-)$ and $π^+ \rightarrow $ $ e^+ ~ν_e ~e^+ e^- $ come into play. While our solution is in conformity with the bounds on the former decay, it remains in tension with $90\%$ CL bounds on the latter. We also discuss other constraints from both collider and non-collider experiments and from electroweak precision data, stability and unitarity. We compute the contributions to the electron and muon $g-2$ up to two loops for our model. We discuss tests of the model in upcoming experiments.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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