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Freeze-in production of FIMP dark matter

Lawrence J. HallInstitute for the Physics and Mathematics of the Universe, University of Tokyo, Kashiwa, 277-8568, JapanKarsten JedamzikLaboratoire de Physique Theorique et Astroparticules, UMR5207-CNRS, Universite Montpellier II, F-34095, Montpellier, FranceJohn March-RussellRudolf Peierls Centre for Theoretical Physics, University of Oxford, 1 Keble Rd., Oxford, OX1 3NP, U.KStephen M. WestRutherford Appleton Laboratory, Chilton, Didcot, OX11 0QX, U.K
2010en
ABI

Annotatsiya

We propose an alternate, calculable mechanism of dark matter genesis, “thermal freeze-in”, involving a Feebly Interacting Massive Particle (FIMP) interacting so feebly with the thermal bath that it never attains thermal equilibrium. As with the conventional “thermal freeze-out” production mechanism, the relic abundance reflects a combination of initial thermal distributions together with particle masses and couplings that can be measured in the laboratory or astrophysically. The freeze-in yield is IR dominated by low temperatures near the FIMP mass and is independent of unknown UV physics, such as the reheat temperature after inflation. Moduli and modulinos of string theory compactifications that receive mass from weak-scale supersymmetry breaking provide implementations of the freeze-in mechanism, as do models that employ Dirac neutrino masses or GUT-scale-suppressed interactions. Experimental signals of freeze-in and FIMPs can be spectacular, including the production of new metastable coloured or charged particles at the LHC as well as the alteration of big bang nucleosynthesis.

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