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Report number arXiv:1810.10905 ; CERN-TH/2018-185 ; CERN-TH-2018-185 ; DESY-18-182 ; PSI-PR-18-11 ; UMN-TH-3801/18 ; FTPI-MINN-18/18 ; UMN-TH-3801/18, FTPI-MINN-18/18 ; IFT-UAM/CSIC-18-081 ; KIAS-P18095 ; KCL-PH-TH/2018-41 ; MPP-2018-239 ; KCL-PH-TH/2018-41, MPP-2018-239 ; CP3-Origins-2018-039 DNRF90
Title Supersymmetric Models in Light of Improved Higgs Mass Calculations
Author(s) Bagnaschi, E. (PSI, Villigen) ; Bahl, H. (Munich, Max Planck Inst.) ; Ellis, J. (King's Coll. London ; NICPB, Tallinn ; CERN) ; Evans, J. (Korea Inst. Advanced Study, Seoul) ; Hahn, T. (Munich, Max Planck Inst.) ; Heinemeyer, S. (Madrid, IFT ; Cantabria Inst. of Phys.) ; Hollik, W. (Munich, Max Planck Inst.) ; Olive, K.A. (Minnesota U., Theor. Phys. Inst.) ; Paßehr, S. (Paris, LPTHE) ; Rzehak, H. (Southern Denmark U., CP3-Origins) ; Sobolev, I.V. (DESY) ; Weiglein, G. (DESY) ; Zheng, J. (Tokyo U.)
Publication 2019-02-19
Imprint 2018-10-25
Number of pages 35
Note 35 pages, 12 figues
In: Eur. Phys. J. C 79 (2019) 149
DOI 10.1140/epjc/s10052-019-6658-y
Subject category hep-ph ; Particle Physics - Phenomenology
Abstract We discuss the parameter spaces of supersymmetry (SUSY) scenarios taking into account the improved Higgs-mass prediction provided by FeynHiggs 2.14.1. Among other improvements, this prediction incorporates three-loop renormalization-group effects and two-loop threshold corrections, and can accommodate three separate mass scales: m_{\tilde q} (for squarks), m_{\tilde g} (for gluinos) and m_{\tilde\chi} (for electroweakinos). Furthermore, it contains an improved treatment of the DRbar scalar top parameters avoiding problems with the conversion to on-shell parameters, that yields more accurate results for large SUSY-breaking scales. We first consider the CMSSM, in which the soft SUSY-breaking parameters m_0 and m_{1/2} are universal at the GUT scale, and then sub-GUT models in which universality is imposed at some lower scale. In both cases, we consider the constraints from the Higgs-boson mass M_h in the bulk of the (m_0, m_{1/2}) plane and also along stop coannihilation strips where sparticle masses may extend into the multi-TeV range. We then consider the minimal anomaly-mediated SUSY-breaking (mAMSB) scenario, in which large sparticle masses are generic. In all these scenarios the substantial improvements between the calculations of M_h in FeynHiggs 2.14.1 and FeynHiggs 2.10.0, which was used in an earlier study, change significantly the preferred portions of the models' parameter spaces. Finally, we consider the pMSSM11, in which sparticle masses may be significantly smaller and we find only small changes in the preferred regions of parameter space.
Copyright/License publication: (License: CC-BY-4.0)
preprint: (License: arXiv nonexclusive-distrib 1.0)

0$} (upper left panel), for \mbox{$\tan \beta = 5$}, \mbox{$\mu > 0$} (upper right panel), for \mbox{$\tan \beta = 5$}, \mbox{$\mu < 0$} (lower left panel), and for \mbox{$\tan \beta = 20$}, \mbox{$\mu > 0$} (lower right panel). The electroweak symmetry-breaking conditions cannot be satisfied in the regions shaded pink in these plots. Contours of~$\Mh$ calculated using \FHnew\ are shown as red solid lines, those using \FHold\ as gray dashed lines. The light orange shaded region corresponds to~\mbox{$\Mh \in [122,128] \gev$} found using \FHnew. The blue strips show the region with~\mbox{$0.06 < \Omega_\chi\, h^2 < 0.2$}." width="200px"/> 0$} (upper left), \mbox{$\tan \beta = 5$}, \mbox{$A_0 = 3\, m_0$} and \mbox{$\mu < 0$} (upper right), \mbox{$\tan \beta = 5$}, \mbox{$A_0 = - 4.2\, m_0$} and \mbox{$\mu > 0$} (lower left), and \mbox{$\tan \beta = 5$}, \mbox{$A_0 = - 4.2\, m_0$} and \mbox{$\mu < 0$} (lower right). The lower horizontal axes {show}~$m_{1/2}$, and the upper horizontal axes show the corresponding values of~$\mneu1$ in~TeV. The blue curves show the mass difference~\mbox{$m_{\tilde t_1} - \mneu1$}, to be read from the left vertical axes. The horizontal light orange shaded band between~\mbox{$\Mh = 122, 128 \gev$} corresponds to {predictions for~$\Mh$ that may be regarded as consistent with experiment.} The other lines show the values of~$\Mh$ calculated using \FHnew\ (red) and \FHold\ (dashed black), to be read from the right vertical axes." width="200px"/> 0$} (left panels), \mbox{$\mu < 0$} (right panels) and \mbox{$\tb = 10$} (upper panels) and \mbox{$\tb = 30$} (lower panels). The lower horizontal axes show~$m_{1/2}$, the blue dashed curves show the value of~$m_0$, to be read from the left vertical axes. The horizontal light orange shaded band between~\mbox{$\Mh = 122, 128 \gev$} corresponds to {predictions for~$\Mh$ that may be regarded as consistent with experiment.} The other lines show the values of~$\Mh$ calculated using \FHnew\ (red) and \FHold\ (dashed black), to be read from the right vertical axes." width="200px"/> Show more plots


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