Status of the scalar singlet dark matter model

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作者
Peter Athron
Csaba Balázs
Torsten Bringmann
Andy Buckley
Marcin Chrząszcz
Jan Conrad
Jonathan M. Cornell
Lars A. Dal
Joakim Edsjö
Ben Farmer
Paul Jackson
Felix Kahlhoefer
Abram Krislock
Anders Kvellestad
James McKay
Farvah Mahmoudi
Gregory D. Martinez
Antje Putze
Are Raklev
Christopher Rogan
Aldo Saavedra
Christopher Savage
Pat Scott
Nicola Serra
Christoph Weniger
Martin White
机构
[1] Monash University,School of Physics and Astronomy
[2] Australian Research Council Centre of Excellence for Particle Physics at the Tera-scale,Department of Physics
[3] Australia,SUPA, School of Physics and Astronomy
[4] University of Oslo,Physik
[5] University of Glasgow,Institut
[6] Universität Zürich,H. Niewodniczański Institute of Nuclear Physics
[7] Polish Academy of Sciences,Oskar Klein Centre for Cosmoparticle Physics
[8] AlbaNova University Centre,Department of Physics
[9] Stockholm University,Department of Physics
[10] McGill University,Department of Physics
[11] University of Adelaide,Department of Physics, Blackett Laboratory
[12] DESY,Theoretical Physics Department
[13] NORDITA,Physics and Astronomy Department
[14] Imperial College London,Department of Physics
[15] Univ Lyon,Centre for Translational Data Science, Faculty of Engineering and Information Technologies, School of Physics
[16] Univ Lyon 1,GRAPPA, Institute of Physics
[17] ENS de Lyon,undefined
[18] CNRS,undefined
[19] Centre de Recherche Astrophysique de Lyon UMR5574,undefined
[20] CERN,undefined
[21] University of California,undefined
[22] LAPTh,undefined
[23] Université de Savoie,undefined
[24] CNRS,undefined
[25] Harvard University,undefined
[26] The University of Sydney,undefined
[27] University of Amsterdam,undefined
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摘要
One of the simplest viable models for dark matter is an additional neutral scalar, stabilised by a Z2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbb {Z}_2$$\end{document} symmetry. Using the GAMBIT package and combining results from four independent samplers, we present Bayesian and frequentist global fits of this model. We vary the singlet mass and coupling along with 13 nuisance parameters, including nuclear uncertainties relevant for direct detection, the local dark matter density, and selected quark masses and couplings. We include the dark matter relic density measured by Planck, direct searches with LUX, PandaX, SuperCDMS and XENON100, limits on invisible Higgs decays from the Large Hadron Collider, searches for high-energy neutrinos from dark matter annihilation in the Sun with IceCube, and searches for gamma rays from annihilation in dwarf galaxies with the Fermi-LAT. Viable solutions remain at couplings of order unity, for singlet masses between the Higgs mass and about 300 GeV, and at masses above ∼\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sim $$\end{document}1 TeV. Only in the latter case can the scalar singlet constitute all of dark matter. Frequentist analysis shows that the low-mass resonance region, where the singlet is about half the mass of the Higgs, can also account for all of dark matter, and remains viable. However, Bayesian considerations show this region to be rather fine-tuned.
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