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Dark Matter and the Baryon Asymmetry of the Universe
High Energy Physics - Phenomenology · Submitted 24 Jun 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim If $m_X \lsi 4.5 B_X $GeV and the annihilation cross sections differ by $\gsi 10%$, this type of scenario naturally explains the observed $\Omega_{DM} \approx 5 \Omega_b$.
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The abstract, sentence by sentence
We present a mechanism to generate the baryon asymmetry of the Universe which preserves the net baryon number created in the Big Bang. If dark matter particles carry baryon number $B_X$, and $\sigma^{\rm annih}_{\bar{X}} < \sigma^{\rm annih}_{X} $, the $\bar{X}$'s freeze out at a higher temperature and have a larger relic density than $X$'s. If $m_X \lsi 4.5 B_X $GeV and the annihilation cross sections differ by $\gsi 10%$, this type of scenario naturally explains the observed $\Omega_{DM} \approx 5 \Omega_b$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a mechanism to generate the baryon asymmetry of the Universe which preserves the net baryon number created in the Big Bang. | contribution 1.00 | 0.88 | 0.40 | asserted 0.99 |
| s1 | If dark matter particles carry baryon number $B_X$, and $\sigma^{\rm annih}_{\bar{X}} < \sigma^{\rm annih}_{X} $, the $\bar{X}$'s freeze out at a higher temperature and have a larger relic density than $X$'s. | method 0.41 | 0.36 | 0.09 | asserted 0.84 |
| s2 | If $m_X \lsi 4.5 B_X $GeV and the annihilation cross sections differ by $\gsi 10%$, this type of scenario naturally explains the observed $\Omega_{DM} \approx 5 \Omega_b$. | result 0.71 | 0.57 | 0.51 | asserted 0.56 |
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The paper
Original abstract
We present a mechanism to generate the baryon asymmetry of the Universe which preserves the net baryon number created in the Big Bang. If dark matter particles carry baryon number $B_X$, and $\sigma^{\rm annih}_{\bar{X}} < \sigma^{\rm annih}_{X} $, the $\bar{X}$'s freeze out at a higher temperature and have a larger relic density than $X$'s. If $m_X \lsi 4.5 B_X $GeV and the annihilation cross sections differ by $\gsi 10%$, this type of scenario naturally explains the observed $\Omega_{DM} \approx 5 \Omega_b$.
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References
How the literature uses it
10 arXiv papers cite this in 10 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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If $m_X \lsi 4.5 B_X $GeV and the annihilation cross sections differ by $\mathcal{O}$(10%) or more, this type of scenario naturally explains the observed $\Omega_{DM} \approx 5 \Omega_b$.
Papers citing it · 2 sentences without a confident label
Cites it as background 8 papers
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Models which utilize the second one could contain asymmetric dark matter [ref] or non-thermal dark matter [ref] .
Asymmetric Dark Matter from Hidden Sector Baryogenesis · Introduction · 0.86
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The ADM scenario has been extensively studied in the literature [ref] .
Asymmetric Dark Matter from Leptogenesis · Introduction · 1.00
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The annihilation of dark matter carrying antibaryon number in Super-Kamiokande, leading to induced nucleon decay, has been previously discussed in the literature, e.g. in the context of hylogenesis models [ref] , as well as a first study for the sexaquark [ref] .
On the cosmology and terrestrial signals of sexaquark dark matter · Antisexaquark annihilation signatures · 0.91
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