2020
DOI: 10.1103/physrevd.101.095005
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Leptogenesis and dark matter from a low scale seesaw mechanism

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Cited by 19 publications
(16 citation statements)
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“…The relation between these intriguing phenomena has been investigated in many works . One of the interesting possibilities is to connect the dark sector and the Standard Model through the RH neutrinos that realise the type I seesaw, which is usually named the neutrino portal scenario [104][105][106][107][108][109][110][111][112][113][114]. Some recent research [104][105][106] shows that dark matter particles can be dominantly produced through the neutrino Yukawa interactions in the seesaw sector non-thermally by the so-called "freeze-in" mechanism [115,116].…”
Section: Introductionmentioning
confidence: 99%
“…The relation between these intriguing phenomena has been investigated in many works . One of the interesting possibilities is to connect the dark sector and the Standard Model through the RH neutrinos that realise the type I seesaw, which is usually named the neutrino portal scenario [104][105][106][107][108][109][110][111][112][113][114]. Some recent research [104][105][106] shows that dark matter particles can be dominantly produced through the neutrino Yukawa interactions in the seesaw sector non-thermally by the so-called "freeze-in" mechanism [115,116].…”
Section: Introductionmentioning
confidence: 99%
“…As the seesaw mechanism involves lepton number violation, it is commonly linked to leptogenesis [24][25][26][27][28][29][30][31][32][33][34] which provides an attractive and minimal origin of the baryon asymmetry in the Universe. Using the observed value of Baryon asymmetry [35], the seesaw parameters can be constrained and related to other cosmological problems like the dark matter [36][37][38][39][40][41][42]. However, standard leptogenesis can hardly be related to collider experiments, as there is a well-known lower bound of RH neutrino mass around 10 9 GeV [43].…”
Section: Contents 1 Introductionmentioning
confidence: 99%
“…Another great mystery unanswered by the SM is that of cosmological dark matter (DM), which is commonly thought to be some kind of massive new particle that is stable on cosmological timescales. Although many DM candidates have been proposed, the most common mechanism to account for their stability is to invent a discrete symmetry, the simplest example being Z 2 , under which the dark matter candidate is odd, while the SM particles are even, where such models may be related to neutrino mass and mixing [24][25][26][27][28][29][30][31][32][33][34][35][36][37][38][39]. Although this approach can explain the mystery of invisible dark matter, accounting for about a quarter of the energy density of the universe [40], the origin of the discrete symmetry such as Z 2 is rarely considered in the literature, but instead is often just imposed, for example as in the case of R-parity in supersymmetry (SUSY).…”
Section: Introductionmentioning
confidence: 99%