RECORD
Nucleosynthesis Constraints on a Massive Gravitino in Neutralino Dark Matter Scenarios
Cosmology and Nongalactic Astrophysics · Submitted 28 Jul 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Discounting this, for m_{1/2} ~ 500 GeV and tan beta = 10 the other light-element abundances impose an upper limit m_{3/2} n_{3/2}/n_\gamma < 3 \times 10^{-12} GeV to < 2 \times 10^{-13} GeV for m_{3/2} = 250 GeV to 1 TeV, which is similar in both the coannihilation and focus-point strips and somewhat weaker for tan beta = 50, particularly for larger m_{1/2}.
The compiled record
The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
Open the compiled record
The abstract, sentence by sentence
The decays of massive gravitinos into neutralino dark matter particles and Standard Model secondaries during or after Big-Bang nucleosynthesis (BBN) may alter the primordial light-element abundances. We present here details of a new suite of codes for evaluating such effects, including a new treatment based on PYTHIA of the evolution of showers induced by hadronic decays of massive, unstable particles such as a gravitino. We also develop an analytical treatment of non-thermal hadron propagation in the early universe, and use this to derive analytical estimates for light-element production and in turn on decaying particle lifetimes and abundances. We then consider specifically the case of an unstable massive gravitino within the constrained minimal supersymmetric extension of the Standard Model (CMSSM). We present upper limits on its possible primordial abundance before decay for different possible gravitino masses, with CMSSM parameters along strips where the lightest neutralino provides all the astrophysical cold dark matter density. We do not find any CMSSM solution to the cosmological Li7 problem for small m_{3/2}. Discounting this, for m_{1/2} ~ 500 GeV and tan beta = 10 the other light-element abundances impose an upper limit m_{3/2} n_{3/2}/n_\gamma < 3 \times 10^{-12} GeV to < 2 \times 10^{-13} GeV for m_{3/2} = 250 GeV to 1 TeV, which is similar in both the coannihilation and focus-point strips and somewhat weaker for tan beta = 50, particularly for larger m_{1/2}. The constraints also weaken in general for larger m_{3/2}, and for m_{3/2} > 3 TeV we find a narrow range of m_{3/2} n_{3/2}/n_\gamma, at values which increase with m_{3/2}, where the Li7 abundance is marginally compatible with the other light-element abundances.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The decays of massive gravitinos into neutralino dark matter particles and Standard Model secondaries during or after Big-Bang nucleosynthesis (BBN) may alter the primordial light-element abundances. | background 1.00 | 0.08 | 0.05 | hedged possibility 1.00 |
| s1 | We present here details of a new suite of codes for evaluating such effects, including a new treatment based on PYTHIA of the evolution of showers induced by hadronic decays of massive, unstable particles such as a gravitino. | method 0.60 | 0.95 | 0.03 | asserted 0.99 |
| s2 | We also develop an analytical treatment of non-thermal hadron propagation in the early universe, and use this to derive analytical estimates for light-element production and in turn on decaying particle lifetimes and abundances. | method 0.85 | 0.96 | 0.04 | asserted 1.00 |
| s3 | We then consider specifically the case of an unstable massive gravitino within the constrained minimal supersymmetric extension of the Standard Model (CMSSM). | contribution 0.88 | 0.67 | 0.03 | asserted 0.74 |
| s4 | We present upper limits on its possible primordial abundance before decay for different possible gravitino masses, with CMSSM parameters along strips where the lightest neutralino provides all the astrophysical cold dark matter density. | result 0.87 | 0.95 | 0.21 | asserted 1.00 |
| s5 | We do not find any CMSSM solution to the cosmological Li7 problem for small m_{3/2}. | result 1.00 | 0.96 | 0.19 | asserted 1.00 |
| s6 | Discounting this, for m_{1/2} ~ 500 GeV and tan beta = 10 the other light-element abundances impose an upper limit m_{3/2} n_{3/2}/n_\gamma < 3 \times 10^{-12} GeV to < 2 \times 10^{-13} GeV for m_{3/2} = 250 GeV to 1 TeV, which is similar in both the coannihilation and focus-point strips and somewhat weaker for tan beta = 50, particularly for larger m_{1/2}. | result 1.00 | 0.95 | 0.35 | asserted 1.00 |
| s7 | The constraints also weaken in general for larger m_{3/2}, and for m_{3/2} > 3 TeV we find a narrow range of m_{3/2} n_{3/2}/n_\gamma, at values which increase with m_{3/2}, where the Li7 abundance is marginally compatible with the other light-element abundances. | result 1.00 | 0.96 | 0.19 | asserted 0.97 |
What was examined, and what was not
- arXiv listing abstract v1
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
The paper
Original abstract
The decays of massive gravitinos into neutralino dark matter particles and Standard Model secondaries during or after Big-Bang nucleosynthesis (BBN) may alter the primordial light-element abundances. We present here details of a new suite of codes for evaluating such effects, including a new treatment based on PYTHIA of the evolution of showers induced by hadronic decays of massive, unstable particles such as a gravitino. We also develop an analytical treatment of non-thermal hadron propagation in the early universe, and use this to derive analytical estimates for light-element production and in turn on decaying particle lifetimes and abundances. We then consider specifically the case of an unstable massive gravitino within the constrained minimal supersymmetric extension of the Standard Model (CMSSM). We present upper limits on its possible primordial abundance before decay for different possible gravitino masses, with CMSSM parameters along strips where the lightest neutralino provides all the astrophysical cold dark matter density. We do not find any CMSSM solution to the cosmological Li7 problem for small m_{3/2}. Discounting this, for m_{1/2} ~ 500 GeV and tan beta = 10 the other light-element abundances impose an upper limit m_{3/2} n_{3/2}/n_\gamma < 3 \times 10^{-12} GeV to < 2 \times 10^{-13} GeV for m_{3/2} = 250 GeV to 1 TeV, which is similar in both the coannihilation and focus-point strips and somewhat weaker for tan beta = 50, particularly for larger m_{1/2}. The constraints also weaken in general for larger m_{3/2}, and for m_{3/2} > 3 TeV we find a narrow range of m_{3/2} n_{3/2}/n_\gamma, at values which increase with m_{3/2}, where the Li7 abundance is marginally compatible with the other light-element abundances.
Human review
References
How later papers used it
47 later papers cite it
1 later paper by other authors is listed below: 1 used its data or values. 2 more papers by the same authors are listed: 2 used its method or tool.
Uses its method or tool 2 of 3 papers with this label · 2 by the same authors
By the same authors
-
Followed this paper's treatments of the hadronic and electromagnetic components of showers induced by heavy-particle decays.
Nuclear Reaction Uncertainties, Massive Gravitino Decays and the Cosmological Lithium Problem (2010) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
-
Followed Appendix B of this paper to write the relation between the mass eigenstates and the interaction eigenstates.
Metastable Charged Sparticles and the Cosmological Li7 Problem (2012) (same authors) · 0.94 · paraphrased: the licence does not allow quoting
Uses its data or values 1 paper
-
Used this paper's cosmological bound of order 10^-14 to require that the reheating temperature be less than 4×10^4.
Gravitino production in a thermal Universe revisited (2016) · 0.92 · paraphrased: the licence does not allow quoting
How the literature uses it
47 arXiv papers cite this in 81 sentences
Papers citing it · 62 sentences without a confident label
Uses its method or tool 3 papers
-
Our treatments of the hadronic and electromagnetic components of the showers induced by heavy-particle decays follow those in [ref] .
Nuclear Reaction Uncertainties, Massive Gravitino Decays and the Cosmological Lithium Problem · Principal Nuclear Reaction Rates · 1.00
-
In this study, we revisit the impact of evaporating black holes on the formation of primordial nuclei, making use of the recent study by Kawasaki et al. (2018), who have used a sophisticated code to study the effects of long-lived particles on BBN [ref] .[For earlier work studying the impact of long-lived decaying particles on BBN, see Refs. [ref] .] In many respects, evaporating black holes alter the predicted light element abundances in ways that are similar to decaying particles.
Constraints on Primordial Black Holes From Big Bang Nucleosynthesis Revisited · The Impact of Evaporating Black Holes on Big Bang Nucleosynthesis · 0.97
-
We presented in [ref] our method of estimating the EM and the hadronic decays of the direct products of the $χ$ decays using the PYTHIA event generator [ref] .
Metastable Charged Sparticles and the Cosmological Li7 Problem · Decays of the NLSP in Gravitino Dark Matter Scenarios · 0.99
Uses its data or values 1 paper
-
In order that the abundance lie within the cosmological bound of order $10^-14$ as given in Ref. [ref] , $T_reh$ should be less than $4×10^4$.
Gravitino production in a thermal Universe revisited · Out of equilibrium production of gravitinos · 0.92
Compares with it 2 papers
-
As in Fig. [ref], the region where the deuterium abundance lies within the favoured range is now also pushed to lower $ζ_3/2$ when $m_3/2 2$ TeV as compared to the results in [ref] , and the region of acceptable 7 abundance extends to lower $ζ_3/2$ when $m_3/2$ is between 2 – 3 TeV.
Nuclear Reaction Uncertainties, Massive Gravitino Decays and the Cosmological Lithium Problem · Principal Nuclear Reaction Rates · 1.00
-
The abundance obtained above can then be compared with the corresponding upper limit of $10^-14$ obtained in Ref. [ref] from various cosmological constraints for $m_3/2∼100$.
Supersymmetric flat directions and resonant gravitino production · Resonant gravitino production · 0.82
Cites it as support 1 paper
-
Decays of the next-to-lightest superparticle occur rapidly via RPV interactions, and thus they do not upset the Big-Bang nucleosynthesis, unlike the $R$-parity conserving case [ref] .
Probing neutrino physics at LHC through R-parity breaking supersymmetry · Dark matter and $R$-parity violating SUSY · 0.96
Cites it as background 8 papers
-
As described in [ref] , non-thermal hadrons $h ∈(p,n)$ are injected into the cosmological baryon/photon plasma by the decay of a heavy particle such as the NLSP, and then interact with the cosmic medium through which they travel.
Nuclear Reaction Uncertainties, Massive Gravitino Decays and the Cosmological Lithium Problem · Principal Nuclear Reaction Rates · 0.87
-
These decays produce electromagnetic energy and hadrons which affect the primordial Big-Bang Nucleosynthesis (BBN) prediction for the abundances of the light nuclei, like D, 4, 3 and 7 [ref] .
GravitinoPack and decays of supersymmetric metastable particles · Introduction · 0.81
-
The light nuclei will interact not only with the CHAMPs during the BBN processes [ref] , but also with the decay products of the CHAMPs in the post-BBN era [ref] .
Big-bang nucleosynthesis with a long-lived charged massive particle including $^4$He spallation processes · Introduction · 0.85
What it cites · 99 sentences without a confident label
Uses the method or tool of 4 papers
-
At high energies $1$ GeV, two other loss mechanisms are important, and our treatment here closely follows that of [ref] .
Hadronic Decay of Late-Decaying Particles and Big-Bang Nucleosynthesis · Energy Losses · 0.99
-
In calculating the relevant gravitino decay rates, we use the interaction Lagrangian given in [ref] :
Electroweak Contributions to Thermal Gravitino Production · Gravitino Decay Amplitudes · 0.96
-
These are treated as in [ref] , but are not dominant when hadronic branchings are significant.
Updated Nucleosynthesis Constraints on Unstable Relic Particles · Interactions with Background Nuclides · 0.98
Uses data or values from 5 papers
-
We adopt the recent revised fit to $3(α,γ)7$ from Cyburt and Davids [ref] .
Evaluation of Modern 3He(alpha,gamma)7Be Data · Rates for Non-Thermal Reactions on Background Light Nuclei · 0.95
-
For fixed values of $tanβ$, the regions of parameter space for which the relic density of neutralinos is computed to lie within the range $0.0975 < Ω_CDM h^2 < 0.1223$ determined by WMAP [ref] and other observations for cold dark matter form narrow strips that foliate the $(m_1/2,m_0)$ plane [ref] .
Proposed Post-LEP Benchmarks for Supersymmetry · Gravitino Decays · 0.83
-
For fixed values of $tanβ$, the regions of parameter space for which the relic density of neutralinos is computed to lie within the range $0.0975 < Ω_CDM h^2 < 0.1223$ determined by WMAP [ref] and other observations for cold dark matter form narrow strips that foliate the $(m_1/2,m_0)$ plane [ref] .
Supersymmetric Dark Matter in Light of WMAP · Gravitino Decays · 0.83
Compares with 4 papers
-
We conclude by commenting on the differences between the amplitudes obtained and used this paper and those given [ref] and [ref] , which are based on the gravitino interaction Lagrangian given in eq.
Supergravity with a Gravitino LSP · Gravitino Decay Amplitudes · 0.99
-
We conclude by commenting on the differences between the amplitudes obtained and used this paper and those given [ref] and [ref] , which are based on the gravitino interaction Lagrangian given in eq.
Big-Bang Nucleosynthesis with Unstable Gravitino and Upper Bound on the Reheating Temperature · Gravitino Decay Amplitudes · 0.99
-
(4.58) of [ref] .
Effects of the Gravitino on the Inflationary Universe · Gravitino Decay Amplitudes · 0.93
Cites as background 7 papers
-
In this case, the gravitino itself would be stable, but the next-to-lightest supersymmetric particle (NLSP) would in general be metastable, and its decays would be subject to the BBN constraints [ref] .
Gravitino Dark Matter in the CMSSM · Introduction · 0.85
-
In this case, the gravitino itself would be stable, but the next-to-lightest supersymmetric particle (NLSP) would in general be metastable, and its decays would be subject to the BBN constraints [ref] .
Supergravity with a Gravitino LSP · Introduction · 0.85
-
In this case, the gravitino itself would be stable, but the next-to-lightest supersymmetric particle (NLSP) would in general be metastable, and its decays would be subject to the BBN constraints [ref] .
SuperWIMP Dark Matter Signals from the Early Universe · Introduction · 0.85
Discussion
Know something about this paper? Leave a comment, or highlight any passage above to comment on it.