论文标题

从弦线中出现的辐射天然超对称性

Radiative natural supersymmetry emergent from the string landscape

论文作者

Baer, Howard, Barger, Vernon, Martinez, Dakotah, Salam, Shadman

论文摘要

在带有通量压实的弦理论中,从真空能量值的离散量对结构形成的拟人选择提供了目前我们对宇宙常数微小而积极值的唯一理解。我们将类似的推理应用于以MSSM为限制为Vacua的多元宇宙的玩具模型,作为低能量有效理论。在这里,人们期望统计选择有利于大型软Susy断裂项,从而导致每个口袋宇宙中弱尺度的衍生值(具有适当的electroweak对称性破坏),这与我们宇宙中所测量的弱尺度不同。相反,保留μ参数的SUSY在对数尺度上均匀选择,这与Sm fermion质量的分布一致:这有利于μ的较小值。弱量表的拟人选择在我们所测量的值的一倍以内 - 为了产生我们所知的复杂核(原子原理),可以根据LHC测量为HIGGS和Sparticle质量提供统计预测。然后,统计选择更常见地导致(辐射驱动){\ IT天然} SUSY模型,或者在标准模型上或精心调整的SUSY模型(例如MSUGRA/CMSSM),分裂,微型切片,传播,扩散,高尺度或PEV SUSY。预测的希格斯和超级粒子光谱可能通过Higgsino对生产在HL-LHC上进行测试,但在具有\ sqrt {s} 〜30-100 TEV的高能量强子山子山子壁上可以测试。

In string theory with flux compactifications, anthropic selection for structure formation from a discretuum of vacuum energy values provides at present our only understanding of the tiny yet positive value of the cosmological constant. We apply similar reasoning to a toy model of the multiverse restricted to vacua with the MSSM as the low energy effective theory. Here, one expects a statistical selection favoring large soft SUSY breaking terms leading to a derived value of the weak scale in each pocket universe (with appropriate electroweak symmetry breaking) which differs from the weak scale as measured in our universe. In contrast, the SUSY preserving μparameter is selected uniformly on a log scale as is consistent with the distribution of SM fermion masses: this favors smaller values of μ. An anthropic selection of the weak scale to within a factor of a few of our measured value -- in order to produce complex nuclei as we know them (atomic principle) -- provides statistical predictions for Higgs and sparticle masses in accord with LHC measurements. The statistical selection then more often leads to (radiatively-driven) {\it natural} SUSY models over the Standard Model or finely-tuned SUSY models such as mSUGRA/CMSSM, split, mini-split, spread, high scale or PeV SUSY. The predicted Higgs and superparticle spectra might be testable at HL-LHC via higgsino pair production but is certainly testable at higher energy hadron colliders with \sqrt{s}~ 30-100 TeV.

扫码加入交流群

加入微信交流群

微信交流群二维码

扫码加入学术交流群,获取更多资源