4.6 Article

Hidden inflaton dark matter

出版社

IOP Publishing Ltd
DOI: 10.1088/1475-7516/2019/03/012

关键词

cosmology of theories beyond the SM; dark matter theory; inflation; particle physics - cosmology connection

资金

  1. DFG [TRR33]
  2. DAAD PPP Kolumbien 2018 project/COLCIENCIAS - DAAD grant [57394560, 110278258747]
  3. Simons foundation
  4. U.K. Science and Technology Facilities Council [ST/J001546/1]
  5. Spanish MINECO [FPA2017-84543-P]
  6. European Union [674896, 690575]
  7. COLCIENCIAS [123365843539 RC FP44842-081-2014]
  8. Universidad Antonio Narino grants [2017239, 2018204]

向作者/读者索取更多资源

If cosmic inflation was driven by an electrically neutral scalar field stable on cosmological time scales, the field necessarily constitutes all or part of dark matter (DM). We study this possibility in a scenario where the inflaton field s resides in a hidden sector, which is coupled to the Standard Model sector through the Higgs portal lambda(hs)s(2) (HH)-H-dagger and non-minimally to gravity via xi(s)s(2)R. We study scenarios where the field s first drives inflation, then reheats the Universe, and later constitutes all DM. We consider two benchmark scenarios where the DM abundance is generated either by production during reheating or via non-thermal freeze-in. In both cases, we take into account all production channels relevant for DM in the mass range from keV to PeV scale. On the inflationary side, we compare the dynamics and the relevant observables in two different but well-motivated theories of gravity (metric and Palatini), discuss multi field effects in case both fields (s and h) were dynamical during inflation, and take into account the non-perturbative nature of particle production during reheating. We find that, depending on the initial conditions for inflation, couplings and the DM mass, the scenario works well especially for large DM masses, 10(2) GeV less than or similar to m(s) less than or similar to 10(6) GeV, although there are also small observationally allowed windows at the keV and MeV scales. We discuss how the model can be tested through astrophysical observations.

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