论文标题

QCD中的暗物质粒子

Dark Matter Particle in QCD

论文作者

Farrar, Glennys R., Wang, Zihui, Xu, Xingchen

论文摘要

我们报告了标准模型中暗物质粒子是稳定,中性,尚未发现的强子的可能性。与当前知识兼容的紧凑型色味旋转旋转singlet sexeaquark(s,uuddss)与当前的知识兼容。 S主要通过耦合强度Alpha_SN的Yukawa相互作用与Baryons相互作用,该耦合强度Alpha_sn,由Omega和Phi Vector Meson介导的质量约为1 GEV。如果存在,则S是非常有吸引力的DM候选人。当宇宙从Quark-Gluon等离子体转变为〜150 MeV时,SDM的遗物丰度(SDM)是建立的,并且与观察到的Omega_dm/Omega_b = 5.3+-0.1;这是一个不空的参数结果,因为相关参数是从QCD中知道的。这种遗物丰度到低温的生存需要分解幅度gtilde <〜2 10^-6,舒适地与理论期望和观察性界限兼容,因为分手振幅被动态抑制,并且较小的数量级。散射横截面可能因天生近似的数量级而有所不同,具体取决于alpha_sn,需要重新分析观察限制。我们使用直接检测实验和宇宙​​学约束来确定alpha_sn的允许区域。对于一系列允许的值,我们预测具有质量偏移〜2 AMU的可检测水平的外来核同位素。在加速器实验中检测SEXAQUARK的最有前途的方法是在相对论重离子碰撞或使用Beam-dump设置的中部地区寻找长度相互交互的中性粒子成分,并搜索缺少粒子生产的证据,这些粒子的产生表现为无抗性的Baryon数字和使用Belle-ii II或可能的gluex gluex at j-lab。

We report on the possibility that the Dark Matter particle is a stable, neutral, as-yet-undiscovered hadron in the standard model. The existence of a compact color-flavor-spin singlet sexaquark (S, uuddss) with mass ~2m_p, is compatible with current knowledge. The S interacts with baryons primarily via a Yukawa interaction of coupling strength alpha_SN, mediated by omega and phi vector mesons having mass ~1 GeV. If it exists, the S is a very attractive DM candidate. The relic abundance of S Dark Matter (SDM) is established when the Universe transitions from the quark-gluon plasma to the hadronic phase at ~150 MeV and is in remarkable agreement with the observed Omega_DM/Omega_b = 5.3+-0.1; this is a no-free-parameters result because the relevant parameters are known from QCD. Survival of this relic abundance to low temperature requires the breakup amplitude gtilde <~ 2 10^-6, comfortably compatible with theory expectations and observational bounds because the breakup amplitude is dynamically suppressed and many orders of magnitude smaller, as we show. The scattering cross section can differ by orders of magnitude from Born approximation, depending on alpha_SN, requiring reanalysis of observational limits. We use direct detection experiments and cosmological constraints to determine the allowed region of alpha_SN. For a range of allowed values, we predict exotic nuclear isotopes at a detectable level with mass offset ~2 amu. The most promising approaches for detecting the sexaquark in accelerator experiments are to search for a long-interaction-length neutral particle component in the central region of relativistic heavy ion collisions or using a beam-dump setup, and to search for evidence of missing particle production characterized by unbalanced baryon number and strangeness using Belle-II or possibly GLUEX at J-Lab.

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