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Realistic Dirac Leptogenesis
High Energy Physics - Phenomenology · Submitted 19 Jun 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This model clearly demonstrates that, contrary to conventional wisdom, neutrinos need not be Majorana in nature in order to help explain the baryon asymmetry of the universe.
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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.
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The abstract, sentence by sentence
We present a model of leptogenesis that preserves lepton number. The model maintains the important feature of more traditional leptogenesis scenarios: the decaying particles that provide the CP violation necessary for baryogenesis also provide the explanation for the smallness of the neutrino Yukawa couplings. This model clearly demonstrates that, contrary to conventional wisdom, neutrinos need not be Majorana in nature in order to help explain the baryon asymmetry of the universe.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a model of leptogenesis that preserves lepton number. | contribution 1.00 | 0.92 | 0.18 | asserted 1.00 |
| s1 | The model maintains the important feature of more traditional leptogenesis scenarios: the decaying particles that provide the CP violation necessary for baryogenesis also provide the explanation for the smallness of the neutrino Yukawa couplings. | contribution 0.62 | 0.38 | 0.13 | asserted 1.00 |
| s2 | This model clearly demonstrates that, contrary to conventional wisdom, neutrinos need not be Majorana in nature in order to help explain the baryon asymmetry of the universe. | interpretation 0.92 | 0.83 | 0.82 | asserted 1.00 |
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The paper
Original abstract
We present a model of leptogenesis that preserves lepton number. The model maintains the important feature of more traditional leptogenesis scenarios: the decaying particles that provide the CP violation necessary for baryogenesis also provide the explanation for the smallness of the neutrino Yukawa couplings. This model clearly demonstrates that, contrary to conventional wisdom, neutrinos need not be Majorana in nature in order to help explain the baryon asymmetry of the universe.
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References
How later papers used it
47 later papers cite it
1 later paper by other authors is listed below: 1 built on it and 1 compared its own results with it. It appears under more than one label.
Builds on it 1 paper
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Presented a variant of this paper's model that achieves conditions on supersymmetry breaking parameters in the neutrino sector avoiding a late non-thermal over-production of LSPs conflicting with the required DM relic density.
Dirac Leptogenesis in extended nMSSM (2008) · 0.92 · paraphrased: the licence does not allow quoting
Compares with it 1 of 4 papers with this label
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Stated that, unlike this paper's extension, its own extension of the MSSM involves only superfields that are singlets under the Standard Model gauge group.
Dirac Leptogenesis in extended nMSSM (2008) · 0.99 · paraphrased: the licence does not allow quoting
How the literature uses it
44 arXiv papers cite this in 55 sentences
Papers citing it · 36 sentences without a confident label
Builds on it 1 paper
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Our aim is to present the conditions on supersymmetry breaking parameters in the neutrino sector avoiding this difficulty, and we present here a variant of the Murayama-Pierce model [ref] which achieves this goal.
Dirac Leptogenesis in extended nMSSM · Introduction · 0.92
Compares with it 4 papers
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This scenario differs from other Dirac leptogenesis models [ref] as it occurs in two steps, described below.
Dirac Leptogenesis in Left-Right Symmetric Models · Dirac Leptogenesis · 0.84
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This is in a way complementary to the proposal in [ref] where an equal and opposite amount of lepton asymmetry were generated in right and left sectors (vanishing net lepton number violation) which were prevented from equilibration by virtue of tiny Dirac Yukawa couplings.
Low scale Dirac leptogenesis and dark matter with observable $\Delta N_{\rm eff}$ · Anomaly Free $B-L$ Model · 1.00
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This is different from flavored-scalar leptogenesis [ref] , where more delicate collider confirmation is needed.
Forbidden neutrinogenesis · Phenomenology · 0.97
Cites it as background 14 papers
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In the above context, a realistic supersymmetric model for Dirac neutrino masses and leptogenesis was proposed in Ref. [ref] , and studied in detail in Refs. [ref] .
Dirac Leptogenesis in extended nMSSM · Introduction · 0.85
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For Dirac neutrinos, there exist essentially two variations of leptogenesis: * Neutrinogenesis [ref] : without ever breaking $B-L$, we let a new particle $σ$ decay out-of-equilibrium into $ν_R$ and left-handed leptons in such a way that a lepton asymmetry is generated in the $ν_R$ that is exactly opposite to an asymmetry in the left-handed leptons: $Δ_ν_R = - Δ_L≠0$.
Observing Dirac neutrinos in the cosmic microwave background · Leptogenesis · 0.84
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In the typical versions of DN mechanism [ref] , the lepton-number asymmetry is generated by heavy particle decays with a non-thermal distribution.
Freeze-in Dirac neutrinogenesis: thermal leptonic CP asymmetry · Introduction · 0.92
Discussion
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