Qiu Yu-Cheng, Tye S-H Henry
Jockey Club Institute for Advanced Study, Hong Kong University of Science and Technology, Hong Kong, S.A.R. China.
Department of Physics, Hong Kong University of Science and Technology, Hong Kong, S.A.R. China.
J High Energy Phys. 2021;2021(1):117. doi: 10.1007/JHEP01(2021)117. Epub 2021 Jan 20.
String theory has no parameter except the string scale , so the Planck scale , the supersymmetry-breaking scale , the electroweak scale as well as the vacuum energy density (cosmological constant) Λ are to be determined dynamically at any local minimum solution in the string theory landscape. Here we consider a model that links the supersymmetric electroweak phenomenology (bottom up) to the string theory motivated flux compactification approach (top down). In this model, supersymmetry is broken by a combination of the racetrack Kähler uplift mechanism, which naturally allows an exponentially small positive Λ in a local minimum, and the anti-D3-brane in the KKLT scenario. In the absence of the Higgs doublets from the supersymmetric standard model, one has either a small Λ or a big enough , but not both. The introduction of the Higgs fields (with their soft terms) allows a small Λ and a big enough simultaneously. Since an exponentially small Λ is statistically preferred (as the properly normalized probability distribution (Λ) diverges at Λ = 0), identifying the observed Λ to the median value Λ yields 100 GeV. We also find that the warped anti-D3-brane tension has a SUSY-breaking scale ∼ 100 while the SUSY-breaking scale that directly correlates with the Higgs fields in the visible sector is ≃ .
弦理论除了弦尺度 外没有其他参数,因此普朗克尺度 、超对称破缺尺度 、电弱尺度 以及真空能量密度(宇宙学常数)Λ 都要在弦理论景观中的任何局部极小解处动态确定。在此,我们考虑一个将超对称电弱现象学(自下而上)与由弦理论推动的通量紧致化方法(自上而下)联系起来的模型。在这个模型中,超对称通过跑道凯勒提升机制(它自然地在局部极小处允许一个指数级小的正Λ)和KKLT情景中的反D3膜的组合而被打破。在没有来自超对称标准模型的希格斯二重态的情况下,要么有一个小的Λ,要么有一个足够大的 ,但不能两者兼得。引入希格斯场(及其软项)允许同时有一个小的Λ和一个足够大的 。由于指数级小的Λ在统计上是更受青睐的(因为适当归一化的概率分布 (Λ) 在Λ = 0 处发散),将观测到的Λ 与中值Λ 等同起来会得到 100 GeV。我们还发现,翘曲的反D3膜张力有一个超对称破缺尺度 ∼ 100 ,而与可见扇区中的希格斯场直接相关的超对称破缺尺度约为 。