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The Heavy Gluino in Natural No-Scale $\cal{F}$-$SU$(5)

High Energy Physics - Phenomenology 2019-10-25 v1 High Energy Physics - Experiment

Abstract

In light of recent 80-137 fb1\rm{fb}^{-1} results at the LHC Run 2 establishing a lower gluino mass limit of 2.25 TeV, we revisit the supersymmetric GUT model Flipped SUSU(5) with extra vector-like particles, known as F\cal{F}-SUSU(5), with vanishing No-Scale Supergravity boundary conditions at the string scale of about 2×10172 \times 10^{17} GeV, including the supersymmetry breaking BμB_{\mu} parameter which is strictly enforced as Bμ=0B_{\mu} = 0. Given the proportional dependence of all model scales on a single parameter M1/2M_{1/2}, No-Scale F\cal{F}-SUSU(5) was shown to possess no electroweak fine-tuning and thus persists as a naturalnatural one-parameter model. In this fresh analysis here, we demand consistency with the measured 125 GeV light Higgs boson mass, though we forgo an upper limit on the lightest neutralino relic density. The resulting phenomenology delivers a gluino mass of M(g~)7.5M(\widetilde{g}) \lesssim 7.5 TeV and a lightest supersymmetric particle (LSP) of M(χ~10)1.6M(\widetilde{\chi}_1^0) \lesssim 1.6 TeV. In order to dilute the relic density down to the WMAP and Planck measurements, we rely upon a single cosmological master coupling λ6\lambda_6.

Keywords

Cite

@article{arxiv.1908.06149,
  title  = {The Heavy Gluino in Natural No-Scale $\cal{F}$-$SU$(5)},
  author = {Thomas Ford and Tianjun Li and James A. Maxin and Dimitri V. Nanopoulos},
  journal= {arXiv preprint arXiv:1908.06149},
  year   = {2019}
}

Comments

7 Pages, 2 Figures, 1 Table