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Bounds on long-lived charged massive particles from Big Bang nucleosynthesis
High Energy Physics - Phenomenology · Submitted 26 Oct 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The analysis yields the surprising result that except for small areas in the particle parameter space conservative constraints on the abundance of decaying charged particles are currently very close to those of neutral particles.
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The abstract, sentence by sentence
The Big Bang nucleosynthesis (BBN) in the presence of charged massive particles (CHAMPs) is studied in detail. All currently known effects due to the existence of bound states between CHAMPs and nuclei, including possible late-time destruction of Li6 and Li7 are included. The study sets conservative bounds on CHAMP abundances in the decay time range 3x10^2 sec - 10^12 sec. It is stressed that the production of Li6 at early times T ~ 10keV is overestimated by a factor ~ 10 when the approximation of the Saha equation for the He4 bound state fraction is utilised. To obtain conservative limits on the abundance of CHAMPs, a Monte-Carlo analysis with ~ 3x10^6 independent BBN runs, varying reaction rates of nineteen different reactions, is performed (see attached erratum, however). The analysis yields the surprising result that except for small areas in the particle parameter space conservative constraints on the abundance of decaying charged particles are currently very close to those of neutral particles. It is shown that, in case a number of heretofore unconsidered reactions may be determined reliably in future, it is conceivable that the limit on CHAMPs in the early Universe could be tightened by orders of magnitude. An ERRATUM gives limits on primordial CHAMP densities when the by Ref. Kamimura et al. recently more accurately determined CHAMP reaction rates are employed.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The Big Bang nucleosynthesis (BBN) in the presence of charged massive particles (CHAMPs) is studied in detail. | contribution 0.93 | 0.86 | 0.03 | asserted 0.97 |
| s1 | All currently known effects due to the existence of bound states between CHAMPs and nuclei, including possible late-time destruction of Li6 and Li7 are included. | contribution 0.54 | 0.55 | 0.03 | asserted 0.98 |
| s2 | The study sets conservative bounds on CHAMP abundances in the decay time range 3x10^2 sec - 10^12 sec. | result 0.82 | 0.94 | 0.32 | asserted 1.00 |
| s3 | It is stressed that the production of Li6 at early times T ~ 10keV is overestimated by a factor ~ 10 when the approximation of the Saha equation for the He4 bound state fraction is utilised. | result 0.96 | 0.71 | 0.06 | asserted 1.00 |
| s4 | To obtain conservative limits on the abundance of CHAMPs, a Monte-Carlo analysis with ~ 3x10^6 independent BBN runs, varying reaction rates of nineteen different reactions, is performed (see attached erratum, however). | method 1.00 | 0.94 | 0.05 | asserted 1.00 |
| s5 | The analysis yields the surprising result that except for small areas in the particle parameter space conservative constraints on the abundance of decaying charged particles are currently very close to those of neutral particles. | result 0.98 | 0.92 | 0.70 | asserted 0.99 |
| s6 | It is shown that, in case a number of heretofore unconsidered reactions may be determined reliably in future, it is conceivable that the limit on CHAMPs in the early Universe could be tightened by orders of magnitude. | future work 0.75 | 0.45 | 0.08 | speculative 0.74 |
| s7 | An ERRATUM gives limits on primordial CHAMP densities when the by Ref. Kamimura et al. recently more accurately determined CHAMP reaction rates are employed. | contribution 0.57 | 0.62 | 0.05 | asserted 0.97 |
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Original abstract
The Big Bang nucleosynthesis (BBN) in the presence of charged massive particles (CHAMPs) is studied in detail. All currently known effects due to the existence of bound states between CHAMPs and nuclei, including possible late-time destruction of Li6 and Li7 are included. The study sets conservative bounds on CHAMP abundances in the decay time range 3x10^2 sec - 10^12 sec. It is stressed that the production of Li6 at early times T ~ 10keV is overestimated by a factor ~ 10 when the approximation of the Saha equation for the He4 bound state fraction is utilised. To obtain conservative limits on the abundance of CHAMPs, a Monte-Carlo analysis with ~ 3x10^6 independent BBN runs, varying reaction rates of nineteen different reactions, is performed (see attached erratum, however). The analysis yields the surprising result that except for small areas in the particle parameter space conservative constraints on the abundance of decaying charged particles are currently very close to those of neutral particles. It is shown that, in case a number of heretofore unconsidered reactions may be determined reliably in future, it is conceivable that the limit on CHAMPs in the early Universe could be tightened by orders of magnitude. An ERRATUM gives limits on primordial CHAMP densities when the by Ref. Kamimura et al. recently more accurately determined CHAMP reaction rates are employed.
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References
How the literature uses it
30 arXiv papers cite this in 48 sentences
Papers citing it · 40 sentences without a confident label
Uses its method or tool 1 paper
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Jedamzik [ref] to include all the latest improvements on decaying relic particles and bound states.
Gravitino dark matter and the lithium primordial abundance within a pre-BBN modified expansion · Calculation procedure · 0.99
Uses its data or values 2 papers
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Refs. [ref] find the excluded regions on the $(τ_NLSP,Ω_NLSPh^2)$ plane for different values of the hadronic branching fraction and two values of the NLSP masses, 100 and 1000 GeV.
Supersymmetric mass spectra for gravitino dark matter with a high reheating temperature · Maximizing the reheating temperature · 0.91
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In addition, adopting $/H|_obs ≲4×10^-11(2.7×10^-10)$ as used in [ref] , the numbers in our Eqs. ([ref]), ([ref]), and ([ref]) change respectively to $6×10^3(10^4)$, $0.87 (0.78)$, and $5.3×10^7 (6.5×10^7)$.
Implications of Catalyzed BBN in the CMSSM with Gravitino Dark Matter · Conclusion · 0.96
Compares with it 1 paper
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This is also confirmed by a direct comparison of our data with Figs. 1 and 2 of the more elaborate CBBN treatment in [ref] for $B_h ≲3×10^-3$ ($≤2.7$, i.e., $≤6$) [ref] at the relevant times of $t≃few×10^3$.
Implications of Catalyzed BBN in the CMSSM with Gravitino Dark Matter · Conclusion · 0.97
Cites it as support 2 papers
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Indeed, it has been shown [ref] that bound-state formation of $τ̃_1^-$ with $^4$He can lead to an overproduction of $^6$Li via the catalyzed BBN (CBBN) reaction $^4$He $X^-$ $+$ D $→$ $^6$Li + $X^-$ [ref] , which has a serious impact on the regions with viable gravitino dark matter [ref] .
Gravitino dark matter in hybrid gauge-gravity models · Gravitino dark matter in hybrid models · 0.96
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Indeed, as discussed in Ref. [ref] , for those branching ratios, the effect of CBBN on is the dominant one in the region which is not already excluded by the D constraint.
The long-lived stau as a thermal relic · Generic constraints on the gravitino-stau scenario · 0.98
Cites it as background 2 papers
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Concerning the inconsistency between the face value of the primordial $^7$Li abundance and the SBBN prediction, various solutions have been discussed from the viewpoint of both astrophysics [ref] and cosmology [ref] .
Big-Bang Nucleosynthesis and Gravitino · Observational light-element abundances · 0.92
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The presence of a long-lived, (color-)charged mediator during BBN can affect the predictions for the primordial abundances of light elements in two ways: through energy release from its decay [ref] and through the formation of bound states with the baryonic matter [ref] .
Top-philic dark matter within and beyond the WIMP paradigm · BBN constraints · 0.88
What it cites · 28 sentences without a confident label
Contests 1 paper
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Though all rates have been determined numerically in the Born approximation in Ref. [ref] , as the Born approximation is likely to fail badly, results become uncertain.
The cosmic 6Li and 7Li problems and BBN with long-lived charged massive particles · Constraints on CHAMPs with long life times · contest 0.75
Uses data or values from 3 papers
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In particular, the Born approximation values of the rates given in Ref. [ref] (shown in Figs. 3 and 4, as well as in Table III and IV of that paper), have been taken as benchmarks.
The cosmic 6Li and 7Li problems and BBN with long-lived charged massive particles · Constraints on CHAMPs with long life times · 0.96
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In order to derive these constraints the rate for 2(4$-X^- ,X^-)^6$Li as given in Ref. [ref] has been utilised.
Stau-catalyzed $^6$Li Production in Big-Bang Nucleosynthesis · Constraints on CHAMPs with intermediate life times · 0.92
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Initial estimates for this enhancemant factor were given at around $6×10^7$ [ref] .
Particle physics catalysis of thermal Big Bang Nucleosynthesis · Introduction · 0.89
Compares with 2 papers
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When these processes are included in the analysis, drastic changes concerning limits on the existence of CHAMPs when compared to those priorly derived [ref] , are obtained.
Stau-catalyzed $^6$Li Production in Big-Bang Nucleosynthesis · Conclusions · 0.90
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When these processes are included in the analysis, drastic changes concerning limits on the existence of CHAMPs when compared to those priorly derived [ref] , are obtained.
Particle physics catalysis of thermal Big Bang Nucleosynthesis · Conclusions · 0.90
Cites as support 1 paper
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Since this is the case for, for example, supersymmetric staus, bound state effects thus still remain very constraining in particular scenarios [ref] .
Particle physics catalysis of thermal Big Bang Nucleosynthesis · Constraints on CHAMPs with intermediate life times · 0.96
Cites as background 5 papers
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Concerning details on the BBN with CHAMPs at late times, the importance of particular reactions, and their evaluation, the reader is referred to the original paper [ref] .
The cosmic 6Li and 7Li problems and BBN with long-lived charged massive particles · Introduction · 0.94
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Though it had been noted already earlier that negatively charged, weak-scale mass particles (CHAMPs) form bound-states with positively charged nuclei towards the end of BBN [ref] , it has only recently been put forward that this may impact considerably the light-element yields synthesized during BBN [ref] .
Particle physics catalysis of thermal Big Bang Nucleosynthesis · Introduction · 0.83
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Though it had been noted already earlier that negatively charged, weak-scale mass particles (CHAMPs) form bound-states with positively charged nuclei towards the end of BBN [ref] , it has only recently been put forward that this may impact considerably the light-element yields synthesized during BBN [ref] .
Big Bang Nucleosynthesis with Long Lived Charged Massive Particles · Introduction · 0.83
Discussion
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