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Quintessence and Spontaneous Leptogenesis
High Energy Physics - Phenomenology · Submitted 5 Dec 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that with a dimension-5 operator ${\partial_\mu Q} J_{B-L}^{\mu}$ suppressed by the Planck mass $M_{pl}$ or the Grand Unification Scale $M_{GUT}$, baryon number asymmetry $n_B/s \sim 10^{-10}$ can be naturally explained {\it via} leptogenesis.
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The abstract, sentence by sentence
We propose in this paper a scenario of spontaneous baryogenesis in cosmological models of Quintessence by introducing a derivative coupling of the Quintessence scalar $Q$ to the baryon current $J_B^{\mu}$ or the current of the baryon number minus lepton number $J_{B-L}^{\mu}$. We find that with a dimension-5 operator ${\partial_\mu Q} J_{B-L}^{\mu}$ suppressed by the Planck mass $M_{pl}$ or the Grand Unification Scale $M_{GUT}$, baryon number asymmetry $n_B/s \sim 10^{-10}$ can be naturally explained {\it via} leptogenesis. We study also the isocurvature baryon number fluctuation generated in our model.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We propose in this paper a scenario of spontaneous baryogenesis in cosmological models of Quintessence by introducing a derivative coupling of the Quintessence scalar $Q$ to the baryon current $J_B^{\mu}$ or the current of the baryon number minus lepton number $J_{B-L}^{\mu}$. | contribution 0.98 | 0.86 | 0.16 | asserted 0.74 |
| s1 | We find that with a dimension-5 operator ${\partial_\mu Q} J_{B-L}^{\mu}$ suppressed by the Planck mass $M_{pl}$ or the Grand Unification Scale $M_{GUT}$, baryon number asymmetry $n_B/s \sim 10^{-10}$ can be naturally explained {\it via} leptogenesis. | result 0.99 | 0.94 | 0.72 | asserted 1.00 |
| s2 | We study also the isocurvature baryon number fluctuation generated in our model. | contribution 1.00 | 0.90 | 0.04 | asserted 0.66 |
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The paper
Original abstract
We propose in this paper a scenario of spontaneous baryogenesis in cosmological models of Quintessence by introducing a derivative coupling of the Quintessence scalar $Q$ to the baryon current $J_B^{\mu}$ or the current of the baryon number minus lepton number $J_{B-L}^{\mu}$. We find that with a dimension-5 operator ${\partial_\mu Q} J_{B-L}^{\mu}$ suppressed by the Planck mass $M_{pl}$ or the Grand Unification Scale $M_{GUT}$, baryon number asymmetry $n_B/s \sim 10^{-10}$ can be naturally explained {\it via} leptogenesis. We study also the isocurvature baryon number fluctuation generated in our model.
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References
How the literature uses it
16 arXiv papers cite this in 23 sentences
Papers citing it · 14 sentences without a confident label
Uses its data or values 1 paper
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In the quintessential baryo/leptogenesis model, $M∼10^8 T_D$ [ref] where $T_D$ is the decoupling temperature of lepton number violating interaction and is around $10^11$ GeV [ref] .
Cosmological CPT violating effect on CMB polarization · The evaluation on the magnitude of corrections in the tracking dark energy model · 0.86
Cites it as background 8 papers
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Several scenarios involving explicit couplings among these species has been proposed in the literature [ref] (see also Ref. [ref] ).
Quintessential Affleck-Dine baryogenesis with non-minimal couplings · Non-minimally coupled Affleck-Dine field · 0.97
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An attractive alternative is spontaneous baryogenesis (leptogenesis) [ref] , where the rotation of a pseudo-Nambu-Goldstone boson induces an effective chemical potential for baryon (lepton) number.
Spontaneous Scoto-leptogenesis · Introduction · 0.93
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A candidate for the scalar $ϕ$ can emerge in a variety of contexts: , inflatons [ref] , flat directions [ref] , radions [ref] , quintessence fields [ref] , scalar curvature [ref] , Higgs fields [ref] , However, scalars with an approximate shift symmetry such as pseudo–Nambu Goldstone bosons (pNGB) are particularly well-motivated in this context [ref] .
Deformation of Axion Potentials: Implications for Spontaneous Baryogenesis, Dark Matter, and Isocurvature Perturbations · Introduction · 0.95
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