2019
DOI: 10.1007/jhep05(2019)072
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Detector-size upper bounds on dark hadron lifetime from cosmology

Abstract: We show that in a confining hidden valley model where the lightest hidden particles are dark hadrons that have mass splittings larger than O(0.1) GeV, if the lightest dark hadron is either stable or decays into Standard Model (SM) hadrons/charged leptons during the big-bang nucleosynthesis (BBN), at least one of the heavier dark hadrons needs to decay into SM particles within O(10) nanosec. Once being produced at collider experiments, this heavier dark hadron is likely to decay within O(1) meter distance, whic… Show more

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Cited by 12 publications
(8 citation statements)
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“…The main process that keeps dark pions in thermal equilibrium with the dark rhos (and hence with the SM) is the pair annihilation ππ → ρρ. This process is fully efficient as long as the temperature is large compared to m ρ −m π , but becomes exponentially suppressed for smaller temperatures [15,20,40]. Provided that the dark ρ mesons are always in thermal equilibrium with the SM, the Boltzmann equation for the dark pion number density n π reads ṅπ…”
Section: Relic Density From Forbidden Annihilationsmentioning
confidence: 99%
“…The main process that keeps dark pions in thermal equilibrium with the dark rhos (and hence with the SM) is the pair annihilation ππ → ρρ. This process is fully efficient as long as the temperature is large compared to m ρ −m π , but becomes exponentially suppressed for smaller temperatures [15,20,40]. Provided that the dark ρ mesons are always in thermal equilibrium with the SM, the Boltzmann equation for the dark pion number density n π reads ṅπ…”
Section: Relic Density From Forbidden Annihilationsmentioning
confidence: 99%
“…Below the scale Λ d , the dark sector confines, which leads to the formation of dark mesons. In particular, this confinement gives rise to three dark pions π 0 d , π + d , π − d , with the U (1) charges 0, +2 and −2, which are stable DM candidates and can arrive at the correct DM relic abundance via Boltzmann-suppressed annihilations into slightly heavier dark mesons [44,45]. These other dark meson species are generically unstable [28].…”
Section: Strongly Interacting Dark Sectormentioning
confidence: 99%
“…Finally, the standard signatures of the FTH scenario are present in the Z 2 scenario as well, including exotic Higgs decays into twin fermions and glueballs which give rise to long-lived particle signatures [18,42,[84][85][86][87][88][89][90], the production of new SM singlet scalar states [88,[91][92][93], and possible signals of the UV completion (see e.g. [94]).…”
Section: Experimental Signaturesmentioning
confidence: 99%