2018
DOI: 10.1103/physrevd.98.095003
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Phenomenology of doublet-triplet fermionic dark matter in nonstandard cosmology and multicomponent dark sectors

Abstract: We consider the doublet-triplet fermionic model in the scheme of the custodial limit when the dark matter (DM) candidate is pure doublet and lies at the electroweak scale. This scheme, despite being an appealing and promising DM model, is severely constrained by the interplay between the DM relic density constraint and the LHC measurement of the Higgs diphoton decay rate. In this work, the DM relic density is considered to arise from either a nonstandard cosmology scenario or as a part of a larger sector encom… Show more

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Cited by 20 publications
(9 citation statements)
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“…This makes it possible to circumvent the well-known ∼100 TeV upper limit on the mass of the DM, based on partial wave unitarity [414] (for related scenarios, see Refs. [415,416,417,341,418,295,278,419,227,420,421,422,39,261,282,423,284,424,288,265,425,426,289,301,300,427,428,429,430,431,432,433,302,434,435,436,437,438,439,290]; for alternative "freeze-in" production of DM in scenarios with a nonstandard expansion phase, see Refs. [440,441,425,442,443,426,289,…”
Section: Consequences For Dark Matter (Authors: a Berlin D Hooper And G Krnjaic)mentioning
confidence: 99%
“…This makes it possible to circumvent the well-known ∼100 TeV upper limit on the mass of the DM, based on partial wave unitarity [414] (for related scenarios, see Refs. [415,416,417,341,418,295,278,419,227,420,421,422,39,261,282,423,284,424,288,265,425,426,289,301,300,427,428,429,430,431,432,433,302,434,435,436,437,438,439,290]; for alternative "freeze-in" production of DM in scenarios with a nonstandard expansion phase, see Refs. [440,441,425,442,443,426,289,…”
Section: Consequences For Dark Matter (Authors: a Berlin D Hooper And G Krnjaic)mentioning
confidence: 99%
“…δL ⊃ χ n Hχ n+1 + h.c., where χ n stands for a fermionic or bosonic n-plet under SU L (2), and DM is the lightest neutral mass eigenstate arising from the mixing of χ n and χ n+1 after the electroweak phase transition (EWPT). These models have been among the archetypical scenarios of DM coupled to the Weak interactions of the SM (WIMPs) [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…enhancement of the cross sections is due to kinematics, the enhancement will remain stable under radiative corrections. Note that in this model, χ 1 forms only a fraction f χ of the total dark matter abundance [43,[72][73][74][75][76][77]:…”
Section: B Direct Detection Of Dark Matter Particlesmentioning
confidence: 99%