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Is light thermal scalar dark matter possible?
High Energy Physics - Phenomenology · Submitted 8 Sep 2021
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim However, we find that two parameter regions still remain, which are the resonant annihilation region and the forbidden annihilation region.
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The abstract, sentence by sentence
We study a light thermal scalar dark matter (DM) model with a light scalar mediator mixed with the standard model Higgs boson, including both the theoretical bounds and the current experimental constraints. The thermal scalar DM with the mass below a few GeV is usually strongly constrained by the observation of CMB and/or indirect detection experiments because the leading annihilation mode is S-wave. However, we find that two parameter regions still remain, which are the resonant annihilation region and the forbidden annihilation region. For the both cases, higher partial waves dominantly contribute to the annihilation at the freeze-out era, and the constraint from the cosmological observation is weaker. We consider typical cases of these regions quantitatively, mainly focusing on the mixing angle and the mass of the new particles. Finally, we also discuss the testability of this model at future experiments.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study a light thermal scalar dark matter (DM) model with a light scalar mediator mixed with the standard model Higgs boson, including both the theoretical bounds and the current experimental constraints. | contribution 1.00 | 0.91 | 0.07 | asserted 0.74 |
| s1 | The thermal scalar DM with the mass below a few GeV is usually strongly constrained by the observation of CMB and/or indirect detection experiments because the leading annihilation mode is S-wave. | background 1.00 | 0.07 | 0.04 | asserted 0.97 |
| s2 | However, we find that two parameter regions still remain, which are the resonant annihilation region and the forbidden annihilation region. | result 1.00 | 0.95 | 0.61 | asserted 1.00 |
| s3 | For the both cases, higher partial waves dominantly contribute to the annihilation at the freeze-out era, and the constraint from the cosmological observation is weaker. | interpretation 0.51 | 0.74 | 0.37 | asserted 1.00 |
| s4 | We consider typical cases of these regions quantitatively, mainly focusing on the mixing angle and the mass of the new particles. | contribution 0.57 | 0.91 | 0.04 | asserted 0.75 |
| s5 | Finally, we also discuss the testability of this model at future experiments. | future work 0.80 | 0.77 | 0.05 | unclear 0.74 |
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The paper
Original abstract
We study a light thermal scalar dark matter (DM) model with a light scalar mediator mixed with the standard model Higgs boson, including both the theoretical bounds and the current experimental constraints. The thermal scalar DM with the mass below a few GeV is usually strongly constrained by the observation of CMB and/or indirect detection experiments because the leading annihilation mode is S-wave. However, we find that two parameter regions still remain, which are the resonant annihilation region and the forbidden annihilation region. For the both cases, higher partial waves dominantly contribute to the annihilation at the freeze-out era, and the constraint from the cosmological observation is weaker. We consider typical cases of these regions quantitatively, mainly focusing on the mixing angle and the mass of the new particles. Finally, we also discuss the testability of this model at future experiments.
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How the literature uses it
6 arXiv papers cite this in 10 sentences
Papers citing it · 6 sentences without a confident label
Compares with it 1 paper
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Similar to the results in [ref] , we have found that scattering collisions are subleading in comparison to the decay process by several orders of magnitude, although our constraint is stronger in comparison to what is found in [ref] .
(sub)GeV Dark Matter in the $U(1)_X$ Higgs Portal Model · Vector DM thermalization · 0.97
Cites it as background 1 paper
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Beyond $s$-wave annihilation, several mechanisms can simultaneously meet CMB constraints and yield the correct relic abundance, such as $p$-wave DM annihilation [ref] , forbidden DM mechanisms [ref] , self-interaction DM [ref] , and other alternatives [ref] .
Light Thermal Dark Matter Beyond $p$-Wave Annihilation in Minimal Higgs Portal Model · Introduction · 0.80
What it cites · 66 sentences without a confident label
Uses data or values from 18 papers
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The most accurate observation of the relic abundance is given by the Planck collaboration [ref] from the observation of the fluctuation of the CMB, which is [equation]
Planck 2018 results. VI. Cosmological parameters · Relic abundance condition · 0.99
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The ATLAS collaboration [ref] gives a constraint on the Higgs invisible decay as $ℬ(h→inv)<0.13$.
Search for invisible Higgs boson decays in vector boson fusion at $\sqrt{s} = 13$ TeV with the ATLAS detector · Higgs boson decay · 0.95
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We show the constraint on mixing angle as the function of $m_H$ in Fig. [ref], and the structure seen around $m_H=0.1`- 0.2$ GeV is due to the background process $K^+ →π^+ π^0$. 2) Visible decay region The NA62 collaboration [ref] also gives the constraint on the process $K^+→π^+ H$ for the visible decay region with almost same magnitude as invisible decay region.
Search for $\pi^0$ decays to invisible particles · $K$ meson decay · 0.91
Cites as background 1 paper
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The theory of the Big Bang nucleosynthesis is well established and the prediction of the fraction ratio of $^1$H, $^2$H, $^3$He and $^4$He matches with the cosmological observations [ref] .
Big Bang Nucleosynthesis: 2015 · Constraint from BBN · 0.93
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