DOI: 10.11606/t.55.2016.tde-29092016-163857
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Resolubilidade global para campos vetoriais no toro n-dimensional

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“…For scalar DM (Fig. 1, right), p-wave suppression of annihilations at late times results in a weak upper bound on y; the bound is likewise exponentially weakened for inelastic DM as the excited state can decay or be thermally depopulated before recombination [22] (not shown in Fig. 1 left).…”
Section: Existing Data Confronts Light Dmmentioning
confidence: 98%
“…For scalar DM (Fig. 1, right), p-wave suppression of annihilations at late times results in a weak upper bound on y; the bound is likewise exponentially weakened for inelastic DM as the excited state can decay or be thermally depopulated before recombination [22] (not shown in Fig. 1 left).…”
Section: Existing Data Confronts Light Dmmentioning
confidence: 98%
“…This qualitatively alters the cosmological phenomenology: although scattering processes still deplete the cosmological population of χ 2 at late times, several experiments can constrain even this small residual abundance. In particular, parts of the parameter space are constrained by considerations of CMB energy injection from χ 1 − χ 2 coannihilation and/or χ 2 decay, while other regions are constrained by χ 2 downscattering in lowthreshold direct detection experiments such as CRESST II [74].…”
Section: Inelastic Dark Matter At Seaquestmentioning
confidence: 99%
“…For MeV scale DM, the splitting can be much smaller ∼ O(keV) to shut off direct detection bounds, but a larger splitting may be necessary in order to sufficiently depopulate the excited state before CMB freeze-out[65], so we conservatively adopt 100 keV.…”
mentioning
confidence: 99%