2021
DOI: 10.1007/jhep01(2021)194
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Single-top final states as a probe of top-flavoured dark matter models at the LHC

Abstract: Models incorporating flavoured dark matter provide an elegant solution to the dark matter problem, evading the tight LHC and direct direction constraints on simple WIMP models. In Dark Minimal Flavour Violation, a simple framework of flavoured dark matter with new sources of flavour violation, the constraints from thermal freeze-out, direct detection experiments, and flavour physics create well-defined benchmark scenarios for these models. We study the LHC phenomenology of four such scenarios, focusing on fina… Show more

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Cited by 11 publications
(6 citation statements)
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“…when there is a sizeable coupling of the ALP with the top quark, provided one interprets 1/Γ as the total lifetime. 9 In the cases where a → 3π dominates, bounds from 4 He overproduction -the dominant constraint in this region -will still hold regardless of the changes in the branching ratios, since only a minimal amount of charged pions is enough for this bound to apply. For even larger masses, ALP decays into hadrons will eventually make its lifetime shorter than a second, making nucleosynthesis constraints harmless.…”
Section: Jhep08(2021)121mentioning
confidence: 99%
“…when there is a sizeable coupling of the ALP with the top quark, provided one interprets 1/Γ as the total lifetime. 9 In the cases where a → 3π dominates, bounds from 4 He overproduction -the dominant constraint in this region -will still hold regardless of the changes in the branching ratios, since only a minimal amount of charged pions is enough for this bound to apply. For even larger masses, ALP decays into hadrons will eventually make its lifetime shorter than a second, making nucleosynthesis constraints harmless.…”
Section: Jhep08(2021)121mentioning
confidence: 99%
“…Note that the limits used in [17] to constrain the Dirac version of top-flavoured DM were based on LHC run 1 data with √ s = 8 TeV. Updated bounds resulting from a recast of 136 fb −1 of LHC run 2 data at √ s = 13 TeV were presented in [23]. In this study we will use the same run 2 limits as in [23] to constrain our model of flavoured Majorana DM.…”
Section: Collider Phenomenologymentioning
confidence: 99%
“…Updated bounds resulting from a recast of 136 fb −1 of LHC run 2 data at √ s = 13 TeV were presented in [23]. In this study we will use the same run 2 limits as in [23] to constrain our model of flavoured Majorana DM.…”
Section: Collider Phenomenologymentioning
confidence: 99%
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