2014
DOI: 10.1103/physrevlett.113.171301
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Mechanism for Thermal Relic Dark Matter of Strongly Interacting Massive Particles

Abstract: We present a new paradigm for achieving thermal relic dark matter. The mechanism arises when a nearly secluded dark sector is thermalized with the standard model after reheating. The freeze-out process is a number-changing 3→2 annihilation of strongly interacting massive particles (SIMPs) in the dark sector, and points to sub-GeV dark matter. The couplings to the visible sector, necessary for maintaining thermal equilibrium with the standard model, imply measurable signals that will allow coverage of a signifi… Show more

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Cited by 542 publications
(609 citation statements)
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“…Several well-motivated classes of models, such as multi-component DM models and models with non-minimal stabilization symmetries, can generate boosted DM as a product of annihilation or decay in nearby clumps of DM. The relevant processes have forms such as multi-component annihilation ψ i ψ j → ψ k ψ [7][8][9], semi-annihilation ψ i ψ j → ψ k φ (where φ is a non-DM state) [7,[10][11][12][13], 3 → 2 self-annihilation [14][15][16], or decay transition ψ i → ψ j + φ. Annihilation of DM is of particular interest, as it is required in the generic scenario that the DM abundance is set by thermal freeze-out.…”
Section: Introductionmentioning
confidence: 99%
“…Several well-motivated classes of models, such as multi-component DM models and models with non-minimal stabilization symmetries, can generate boosted DM as a product of annihilation or decay in nearby clumps of DM. The relevant processes have forms such as multi-component annihilation ψ i ψ j → ψ k ψ [7][8][9], semi-annihilation ψ i ψ j → ψ k φ (where φ is a non-DM state) [7,[10][11][12][13], 3 → 2 self-annihilation [14][15][16], or decay transition ψ i → ψ j + φ. Annihilation of DM is of particular interest, as it is required in the generic scenario that the DM abundance is set by thermal freeze-out.…”
Section: Introductionmentioning
confidence: 99%
“…[5], we assume DM begins in thermal equilibrium, has its number diluted through 2-to-2 annihilations, and has a temperature that tracks the photon temperature (for studies that relax at least one of these assumptions see for example Refs. [14][15][16][17][18][19][20][21][22][23][24][25][26][27]). We consider the presence of two states charged under the symmetry that stabilizes DM: χ and ψ, where m χ < m ψ and χ is DM.…”
mentioning
confidence: 99%
“…For example, the states of a strongly-coupled hidden sector provide a natural context [90] for strongly-interacting massive particle (SIMP) dark matter [91,92] models, in which 3 → 2 processes rather than 2 → 2 processes play a dominant role in determining the dark-matter abundance. Indeed, a number of explicit models along these lines have been constructed [93][94][95][96].…”
Section: Discussionmentioning
confidence: 99%