Author:
Bechtle Philip,Bringmann Torsten,Desch Klaus,Dreiner Herbi,Hamer Matthias,Hensel Carsten,Krämer Michael,Nguyen Nelly,Porod Werner,Prudent Xavier,Sarrazin Björn,Uhlenbrock Mathias,Wienemann Peter
Abstract
Abstract
We perform global fits to the parameters of the Constrained Minimal Super-symmetric Standard Model (CMSSM) and to a variant with non-universal Higgs masses (NUHM1). In addition to constraints from low-energy precision observables and the cosmological dark matter density, we take into account the LHC exclusions from searches in jets plus missing transverse energy signatures with about 5 fb−1 of integrated luminosity. We also include the most recent upper bound on the branching ratio B
s
→ μμ from LHCb. Furthermore, constraints from and implications for direct and indirect dark matter searches are discussed. The best fit of the CMSSM prefers a light Higgs boson just above the experimentally excluded mass. We find that the description of the low-energy observables, (g − 2)
μ
in particular, and the non-observation of SUSY at the LHC become more and more incompatible within the CMSSM. A potential SM-like Higgs boson with mass around 126 GeV can barely be accommodated. Values for
$ \mathcal{B}\left( {{B_{\text{s}}} \to \mu \mu } \right) $
just around the Standard Model prediction are naturally expected in the best fit region. The most-preferred region is not yet affected by limits on direct WIMP searches, but the next generation of experiments will probe this region. Finally, we discuss implications from fine-tuning for the best fit regions.
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
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