2018
DOI: 10.1140/epjc/s10052-018-6314-y
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Impact of vacuum stability, perturbativity and XENON1T on global fits of $$\mathbb {Z}_2$$ and $$\mathbb {Z}_3$$ scalar singlet dark matter

Abstract: Scalar singlet dark matter is one of the simplest and most predictive realisations of the WIMP (weakly-interacting massive particle) idea. Although the model is constrained from all directions by the latest experimental data, it still has viable regions of parameter space. Another compelling aspect of scalar singlets is their ability to stabilise the electroweak vacuum. Indeed, models of scalar dark matter are not low-energy effective theories, but can be valid all the way to the Planck scale. Using the GAMBIT… Show more

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Cited by 93 publications
(91 citation statements)
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“…Previously global fits of DM models, e.g., Ref. [21,22], included at most parametric uncertainties. We can now, however, incorporate coherently all major sources of uncertainty in DD experiments in official limits and global fits.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Previously global fits of DM models, e.g., Ref. [21,22], included at most parametric uncertainties. We can now, however, incorporate coherently all major sources of uncertainty in DD experiments in official limits and global fits.…”
Section: Discussionmentioning
confidence: 99%
“…The number of terms in the sum is equal to the number of unique ways of partitioning q into any number of smaller terms, i.e., the partition function of q. The first ten partitions are 1,2,3,5,7,11,15,22,30 and 42, and, asymptotically, the number of partitions grows exponentially with q. The formula allows us to express complicated moments of a multinomial in terms of simpler ones; in this regard, it is similar to Wick's theorem for Gaussian moments.…”
Section: A Averaged Poisson Likelihoodmentioning
confidence: 99%
“…A global likelihood fit of the Z 3 singlet dark matter was recently made with the GAM-BIT code [79]. This study did not, however, take into account the improvements included in this work, in particular refined unitarity bounds and treatment of early kinetic decoupling.…”
Section: Introductionmentioning
confidence: 99%
“…However, such a term can be removed by performing a constant shift in S which also redefines µ 2 S , µ 2 Φ , µ 3 , g S and µ ΦS . 1 In writing the above Lagrangians, we have assumed that these parameters are defined after a constant shift in S. If we set µ 3 = g S = µ ΦS = 0, we can see that the above Lagrangian becomes Z 2 symmetric under S → −S, i.e., it is even in S. In this case, the fermion DM ψ is decoupled and becomes a hidden DM candidate, whereas the scalar S serves as a new DM candidate and reproduces the scalar Higgs portal model [36,[72][73][74][75][76][77][78][79][80][81].…”
Section: Singlet Fermion Dark Matter Modelmentioning
confidence: 94%