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The abundance of relativistic axions in a flaton model of Peccei-Quinn symmetry
High Energy Physics - Phenomenology · Submitted 14 Aug 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The DFSZ case is allowed in a significant region of parameter space, and will provide a possible explanation for any future detection of nonzero $\delta N_\nu$.
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The abstract, sentence by sentence
Flaton models of Peccei-Quinn symmetry have good particle physics motivation, and are likely to cause thermal inflation leading to a well-defined cosmology. They can solve the $\mu$ problem, and generate viable neutrino masses. Canonical flaton models predict an axion decay constant F_a of order 10^{10} GeV and generic flaton models give F_a of order 10^9 GeV as required by observation. The axion is a good candidate for cold dark matter in all cases, because its density is diluted by flaton decay if F_a is bigger than 10^{12} GeV. In addition to the dark matter axions, a population of relativistic axions is produced by flaton decay, which at nucleosynthesis is equivalent to some number \delta N_\nu of extra neutrino species. Focussing on the canonical model, containing three flaton particles and two flatinos, we evaluate all of the flaton-flatino-axion interactions and the corresponding axionic decay rates. They are compared with the dominant hadronic decay rates, for both DFSZ and KSVZ models. These formulas provide the basis for a precise calculation of the equivalent \delta N_\nu in terms of the parameters (masses and couplings). The KSVZ case is probably already ruled out by the existing bound \delta N_\nu\lsim 1. The DFSZ case is allowed in a significant region of parameter space, and will provide a possible explanation for any future detection of nonzero $\delta N_\nu$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Flaton models of Peccei-Quinn symmetry have good particle physics motivation, and are likely to cause thermal inflation leading to a well-defined cosmology. | background 1.00 | 0.08 | 0.04 | hedged possibility 0.95 |
| s1 | They can solve the $\mu$ problem, and generate viable neutrino masses. | background 0.97 | 0.08 | 0.03 | hedged possibility 0.88 |
| s2 | Canonical flaton models predict an axion decay constant F_a of order 10^{10} GeV and generic flaton models give F_a of order 10^9 GeV as required by observation. | background 0.81 | 0.17 | 0.06 | asserted 0.99 |
| s3 | The axion is a good candidate for cold dark matter in all cases, because its density is diluted by flaton decay if F_a is bigger than 10^{12} GeV. | background 0.50 | 0.17 | 0.07 | asserted 0.97 |
| s4 | In addition to the dark matter axions, a population of relativistic axions is produced by flaton decay, which at nucleosynthesis is equivalent to some number \delta N_\nu of extra neutrino species. | contribution 0.36 | 0.28 | 0.12 | asserted 1.00 |
| s5 | Focussing on the canonical model, containing three flaton particles and two flatinos, we evaluate all of the flaton-flatino-axion interactions and the corresponding axionic decay rates. | method 0.68 | 0.93 | 0.04 | asserted 0.98 |
| s6 | They are compared with the dominant hadronic decay rates, for both DFSZ and KSVZ models. | method 0.91 | 0.80 | 0.03 | asserted 0.95 |
| s7 | These formulas provide the basis for a precise calculation of the equivalent \delta N_\nu in terms of the parameters (masses and couplings). | method 0.58 | 0.81 | 0.08 | asserted 1.00 |
| s8 | The KSVZ case is probably already ruled out by the existing bound \delta N_\nu\lsim 1. | result 0.66 | 0.47 | 0.19 | hedged possibility 0.97 |
| s9 | The DFSZ case is allowed in a significant region of parameter space, and will provide a possible explanation for any future detection of nonzero $\delta N_\nu$. | interpretation 0.82 | 0.67 | 0.38 | hedged possibility 0.85 |
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Original abstract
Flaton models of Peccei-Quinn symmetry have good particle physics motivation, and are likely to cause thermal inflation leading to a well-defined cosmology. They can solve the $\mu$ problem, and generate viable neutrino masses. Canonical flaton models predict an axion decay constant F_a of order 10^{10} GeV and generic flaton models give F_a of order 10^9 GeV as required by observation. The axion is a good candidate for cold dark matter in all cases, because its density is diluted by flaton decay if F_a is bigger than 10^{12} GeV. In addition to the dark matter axions, a population of relativistic axions is produced by flaton decay, which at nucleosynthesis is equivalent to some number \delta N_\nu of extra neutrino species. Focussing on the canonical model, containing three flaton particles and two flatinos, we evaluate all of the flaton-flatino-axion interactions and the corresponding axionic decay rates. They are compared with the dominant hadronic decay rates, for both DFSZ and KSVZ models. These formulas provide the basis for a precise calculation of the equivalent \delta N_\nu in terms of the parameters (masses and couplings). The KSVZ case is probably already ruled out by the existing bound \delta N_\nu\lsim 1. The DFSZ case is allowed in a significant region of parameter space, and will provide a possible explanation for any future detection of nonzero $\delta N_\nu$.
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References
How the literature uses it
5 arXiv papers cite this in 11 sentences
Papers citing it · 7 sentences without a confident label
Compares with it 1 paper
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Our model, though simpler, has much in common with the multi-field thermal inflation axion models studied in Refs. [ref] , and our baryogenesis scenario would probably work in those models too, but there are at least two important differences.
Thermal inflation, baryogenesis and axions · Comparison with multi-field thermal inflation axion models · 0.98
Cites it as background 3 papers
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Various explanations for $Δ∼1$ have been explored in the literature invoking, e.g., light sterile neutrinos [ref] , other light species [ref] , neutrino asymmetries [ref] , or decays of heavy particles [ref] .
Dark radiation and dark matter in supersymmetric axion models with high reheating temperature · Introduction · 0.97
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The dynamics of the saxion and its cosmological implications were discussed in Refs. [ref] .
Dynamics of oscillating scalar field in thermal environment · Peccei-Quinn scalar · 0.96
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(Thermal inflation in the context of PQ symmetry breaking was discussed in Refs. [ref] .) All the dangerous relics such as the gravitino and axino are diluted away.
Peccei-Quinn extended gauge-mediation model with vector-like matter · The saxion trapped at the origin · 0.84
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