One-Zero Neutrino Textures and Resonant Type-II Leptogenesis: Flavor-Resolved Thermal Evolution and Baryon Asymmetry
Pith reviewed 2026-05-20 16:44 UTC · model grok-4.3
The pith
One-zero neutrino textures remain compatible with oscillation data while generating the observed baryon asymmetry through resonant Type-II leptogenesis.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We show that several one-zero textures remain compatible with neutrino oscillation data while simultaneously generating sizable CP asymmetries through resonant enhancement. We further investigate the thermal evolution of the generated asymmetry using Boltzmann equations and demonstrate the freeze-out behavior of the baryon asymmetry. Extending the analysis to a flavor-resolved framework, we study the separate evolution of electron, muon, and tau asymmetries and show that flavor-dependent washout effects play a crucial role in determining the final baryon asymmetry. Our analysis establishes a direct connection between neutrino flavor textures, resonant thermal leptogenesis, and flavor-depend
What carries the argument
One-zero neutrino mass textures realized in a two-triplet scalar Type-II seesaw, analyzed through flavor-resolved Boltzmann equations that track the separate thermal evolution and washout of electron, muon, and tau lepton asymmetries.
If this is right
- Several one-zero neutrino textures fit both current oscillation measurements and produce sufficient CP asymmetry under resonant conditions.
- Resonant leptogenesis remains viable for these textures in both hierarchical and resonant regimes of the two-triplet model.
- Flavor-dependent washout effects must be tracked separately because they control the freeze-out value of the baryon asymmetry.
- The thermal evolution shows clear freeze-out of the generated asymmetry once the relevant scalars decay and interactions decouple.
- A direct link exists between the choice of neutrino texture and the flavor-specific baryogenesis dynamics.
Where Pith is reading between the lines
- The same flavor-resolved tracking could be applied to other seesaw realizations to test whether washout differences persist across models.
- Confirmation of a viable one-zero texture would tighten the allowed range for the scalar triplet masses and couplings in the early universe.
- If oscillation experiments further restrict the mixing parameters, the set of textures that survive could be used to predict the sign or magnitude of the final asymmetry.
- The approach suggests that ignoring flavor resolution in similar calculations risks misestimating the required CP asymmetry strength.
Load-bearing premise
The resonant enhancement of the CP asymmetry in the two-triplet Type-II seesaw can be reliably captured by the standard Boltzmann equations without additional non-thermal or flavor-off-diagonal effects that would alter the freeze-out behavior.
What would settle it
A complete scan over the neutrino parameter space that finds no one-zero texture simultaneously consistent with oscillation data and able to produce a final baryon asymmetry in the observed range after flavor-resolved evolution would falsify the central viability result.
Figures
read the original abstract
We investigate the viability of one-zero neutrino mass textures within the framework of resonant Type-II leptogenesis. Considering a two-triplet scalar realization of the Type-II seesaw mechanism, we analyze the compatibility between neutrino texture structures, CP asymmetry generation, and the observed baryon asymmetry of the Universe. We perform extensive numerical scans over the neutrino parameter space and classify the phenomenologically viable one-zero textures under both hierarchical and resonant leptogenesis scenarios. We show that several one-zero textures remain compatible with neutrino oscillation data while simultaneously generating sizable CP asymmetries through resonant enhancement. We further investigate the thermal evolution of the generated asymmetry using Boltzmann equations and demonstrate the freeze-out behavior of the baryon asymmetry. Extending the analysis to a flavor-resolved framework, we study the separate evolution of electron, muon, and tau asymmetries and show that flavor-dependent washout effects play a crucial role in determining the final baryon asymmetry. Our analysis establishes a direct connection between neutrino flavor textures, resonant thermal leptogenesis, and flavor-dependent baryogenesis dynamics.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript investigates one-zero neutrino mass textures in a two-triplet scalar realization of the Type-II seesaw, performing numerical scans over neutrino parameter space to identify textures compatible with oscillation data that simultaneously generate the observed baryon asymmetry via resonant leptogenesis. It analyzes CP asymmetry generation through resonant enhancement, evolves the asymmetry using flavor-resolved Boltzmann equations, and demonstrates freeze-out behavior with emphasis on flavor-dependent washout effects in electron, muon, and tau channels.
Significance. If the central results hold, the work establishes a phenomenological bridge between specific neutrino mass matrix zero textures and successful resonant Type-II leptogenesis, with the flavor-resolved treatment providing a useful refinement over single-flavor approximations. The numerical classification of viable textures under both hierarchical and resonant scenarios adds concrete constraints that could be tested against upcoming neutrino data and baryon asymmetry measurements.
major comments (1)
- [Thermal evolution and Boltzmann equations section (around the flavor-resolved framework discussion)] The thermal evolution analysis relies on standard Boltzmann equations to compute the final baryon asymmetry from the resonant CP asymmetry in the two-triplet model. In the resonant regime (where triplet mass splitting is comparable to decay widths), this approach implicitly neglects coherent oscillations between the triplets and possible flavor-off-diagonal terms in the density matrix that can modify washout and freeze-out dynamics. An explicit justification or cross-check against the density-matrix formalism is required to support the claim that several one-zero textures produce the observed Y_B.
minor comments (2)
- [Abstract and numerical results section] The abstract states that 'extensive numerical scans' were performed and viable textures identified, but the manuscript should include a brief description of the scan ranges, priors on CP phases, and any criteria used to avoid post-selection bias in the texture classification.
- [Introduction or neutrino textures section] Notation for the one-zero textures (e.g., which specific matrix element is set to zero) should be defined explicitly with a table or equation early in the text for clarity when discussing compatibility with oscillation data.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for the constructive comment on the thermal evolution section. We address the point below and will incorporate revisions to strengthen the presentation.
read point-by-point responses
-
Referee: [Thermal evolution and Boltzmann equations section (around the flavor-resolved framework discussion)] The thermal evolution analysis relies on standard Boltzmann equations to compute the final baryon asymmetry from the resonant CP asymmetry in the two-triplet model. In the resonant regime (where triplet mass splitting is comparable to decay widths), this approach implicitly neglects coherent oscillations between the triplets and possible flavor-off-diagonal terms in the density matrix that can modify washout and freeze-out dynamics. An explicit justification or cross-check against the density-matrix formalism is required to support the claim that several one-zero textures produce the observed Y_B.
Authors: We thank the referee for highlighting this subtlety of the resonant regime. The CP asymmetry in our work is computed with the standard resonant formula that incorporates the mass splitting and decay widths, thereby capturing the leading resonant enhancement. The subsequent evolution employs flavor-resolved Boltzmann equations, which is the standard approach in Type-II leptogenesis studies with scalar triplets. While a full density-matrix treatment would include coherent oscillations and off-diagonal terms, these effects are sub-dominant for the mass splittings and parameter ranges explored in our viable textures, where flavor-diagonal washout dominates the freeze-out. To address the comment directly, we will add a concise justification paragraph in the revised thermal evolution section, supported by references to comparable analyses in the literature that employ the same Boltzmann framework under resonant conditions. This addition will explicitly discuss the regime of validity and why the neglected terms do not alter the classification of viable one-zero textures or the generated Y_B. revision: yes
Circularity Check
No significant circularity; derivation relies on external data and standard methods
full rationale
The paper performs numerical scans over neutrino parameter space to classify one-zero textures compatible with oscillation data, then computes CP asymmetries and baryon asymmetry evolution via Boltzmann equations in a flavor-resolved framework. This uses external benchmarks (neutrino oscillation parameters and observed baryon asymmetry) and standard leptogenesis techniques without reducing the final Y_B to a fitted parameter by construction or depending on a self-citation chain for the core result. The thermal freeze-out and flavor washout analysis follows directly from the model inputs and equations, rendering the chain self-contained.
Axiom & Free-Parameter Ledger
free parameters (2)
- Neutrino mass matrix zero position and CP phases
- Triplet scalar masses and couplings
axioms (2)
- domain assumption The standard Boltzmann equations accurately describe the thermal evolution of lepton asymmetries in the presence of resonant enhancement.
- standard math Sphaleron processes convert the lepton asymmetry into the observed baryon asymmetry with the usual efficiency factor.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We perform extensive numerical scans over the neutrino parameter space and classify the phenomenologically viable one-zero textures under both hierarchical and resonant leptogenesis scenarios.
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The flavored Boltzmann equations can be written schematically as dY_Δα/dz = −ϵ_α D(z)(Y_Δ − Y_eq_Δ) − W_α(z) Y_Δα
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Evidence for Oscillation of Atmo- spheric Neutrinos,
Y. Fukuda et al. [Super-Kamiokande Collaboration], “Evidence for Oscillation of Atmo- spheric Neutrinos,” Phys. Rev. Lett.81, 1562 (1998)
work page 1998
-
[2]
Direct Evidence for Neutrino Flavor Transfor- mation from Neutral Current Interactions,
Q. R. Ahmad et al. [SNO Collaboration], “Direct Evidence for Neutrino Flavor Transfor- mation from Neutral Current Interactions,” Phys. Rev. Lett.89, 011301 (2002)
work page 2002
-
[3]
First Results from KamLAND: Evidence for Reactor Antineutrino Disappearance,
K. Eguchi et al. [KamLAND Collaboration], “First Results from KamLAND: Evidence for Reactor Antineutrino Disappearance,” Phys. Rev. Lett.90, 021802 (2003)
work page 2003
-
[4]
Observation of Electron-Antineutrino Disap- pearance at Daya Bay,
F. P. An et al. [Daya Bay Collaboration], “Observation of Electron-Antineutrino Disap- pearance at Daya Bay,” Phys. Rev. Lett.108, 171803 (2012)
work page 2012
-
[5]
Indication of Electron Neutrino Appearance from an Accelerator-produced Off-axis Muon Neutrino Beam,
K. Abe et al. [T2K Collaboration], “Indication of Electron Neutrino Appearance from an Accelerator-produced Off-axis Muon Neutrino Beam,” Phys. Rev. Lett.107, 041801 (2011)
work page 2011
-
[6]
Planck 2018 results. VI. Cosmological parameters
N. Aghanim et al. [Planck Collaboration], “Planck 2018 Results. VI. Cosmologi- cal Parameters,” Astron. Astrophys.641, A6 (2020) doi:10.1051/0004-6361/201833910 [arXiv:1807.06209 [astro-ph.CO]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1051/0004-6361/201833910 2018
-
[7]
mu -¿ e gamma at a Rate of One Out of 1-Billion Muon Decays?
P. Minkowski, “mu -¿ e gamma at a Rate of One Out of 1-Billion Muon Decays?” Phys. Lett. B67, 421 (1977)
work page 1977
-
[8]
Horizontal Symmetry and Masses of Neutrinos,
T. Yanagida, “Horizontal Symmetry and Masses of Neutrinos,” Prog. Theor. Phys.64, 1103 (1980)
work page 1980
-
[9]
The Family Group in Grand Unified Theories
M. Gell-Mann, P. Ramond and R. Slansky, “The Family Group in Grand Unified Theories,” inSupergravity, edited by P. van Nieuwenhuizen and D. Z. Freedman, North-Holland, Amsterdam (1979), pp. 315–321 [arXiv:hep-ph/9809459]
work page internal anchor Pith review Pith/arXiv arXiv 1979
-
[10]
Neutrino Mass and Spontaneous Parity Violation,
R. N. Mohapatra and G. Senjanovic, “Neutrino Mass and Spontaneous Parity Violation,” Phys. Rev. Lett.44, 912 (1980)
work page 1980
-
[11]
Neutrino Masses in SU(2) x U(1) Theories,
J. Schechter and J. W. F. Valle, “Neutrino Masses in SU(2) x U(1) Theories,” Phys. Rev. D22, 2227 (1980)
work page 1980
-
[12]
Neutrino Mass Problem and Gauge Hierarchy,
M. Magg and C. Wetterich, “Neutrino Mass Problem and Gauge Hierarchy,” Phys. Lett. B94, 61 (1980)
work page 1980
-
[13]
Proton Lifetime and Fermion Masses in an SO(10) Model,
G. Lazarides, Q. Shafi and C. Wetterich, “Proton Lifetime and Fermion Masses in an SO(10) Model,” Nucl. Phys. B181, 287 (1981)
work page 1981
-
[14]
Neutrino Masses and Mixings in Gauge Models with Spontaneous Parity Violation,
R. N. Mohapatra and G. Senjanovic, “Neutrino Masses and Mixings in Gauge Models with Spontaneous Parity Violation,” Phys. Rev. D23, 165 (1981)
work page 1981
-
[15]
Phenomenology of Type-II Seesaw Models,
E. J. Chun et al., “Phenomenology of Type-II Seesaw Models,” Phys. Rev. D66, 073003 (2002). 18
work page 2002
-
[16]
Zeroes of the Neutrino Mass Matrix
P. H. Frampton, S. L. Glashow and D. Marfatia, “Zeroes of the Neutrino Mass Matrix,” Phys. Lett. B536, 79 (2002) doi:10.1016/S0370-2693(02)01817-8 [arXiv:hep-ph/0201008]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/s0370-2693(02)01817-8 2002
-
[17]
Texture Zeros and Majorana Phases of the Neutrino Mass Matrix
Z. z. Xing, “Texture Zeros and Majorana Phases of the Neutrino Mass Matrix,” Phys. Lett. B530, 159 (2002) doi:10.1016/S0370-2693(02)01354-0 [arXiv:hep-ph/0201151]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/s0370-2693(02)01354-0 2002
-
[18]
W. L. Guo and Z. z. Xing, “Implications of the KamLAND Measurement on the Lepton Flavor Mixing Matrix and the Neutrino Mass Matrix,” Phys. Rev. D67, 053002 (2003) doi:10.1103/PhysRevD.67.053002 [arXiv:hep-ph/0212142]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.67.053002 2003
-
[19]
Phenomenology of Two-Texture Zero Neutrino Mass Matrices
S. Dev, S. Kumar, S. Verma and S. Gupta, “Phenomenology of Two Texture Zero Neu- trino Mass Matrices,” Phys. Rev. D76, 013002 (2007) doi:10.1103/PhysRevD.76.013002 [arXiv:hep-ph/0612102]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.76.013002 2007
-
[20]
Zero minors of the neutrino mass matrix
E. I. Lashin and N. Chamoun, “Zero Textures of the Neutrino Mass Matrix from Cyclic Family Symmetry,” Phys. Rev. D78, 073002 (2008) doi:10.1103/PhysRevD.78.073002 [arXiv:0708.2423 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.78.073002 2008
-
[21]
Fine-tuning and naturalness issues in the two-zero neutrino mass textures
D. Meloni and G. Blankenburg, “Fine-Tuning and Naturalness Issues in the Two-Zero Neu- trino Mass Textures,” Nucl. Phys. B867, 749 (2013) doi:10.1016/j.nuclphysb.2012.10.019 [arXiv:1204.2706 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/j.nuclphysb.2012.10.019 2013
-
[22]
A complete survey of texture zeros in the lepton mass matrices
P. O. Ludl and W. Grimus, “A Complete Survey of Texture Zeros in the Lepton Mass Matrices,” JHEP1407, 090 (2014) doi:10.1007/JHEP07(2014)090 [arXiv:1406.3546 [hep- ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep07(2014)090 2014
-
[23]
J. Liao, D. Marfatia and K. Whisnant, “Texture and Cofactor Zeros of the Neutrino Mass Matrix,” JHEP1409, 013 (2014) doi:10.1007/JHEP09(2014)013 [arXiv:1407.2636 [hep- ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep09(2014)013 2014
-
[24]
Turbulence and the Navier-Stokes equations
D. Singh, A. Ahuja and M. Gupta, “Texture One-Zero Neutrino Mass Matrices and Current Experimental Tests,” Phys. Rev. D76, 013006 (2007) doi:10.1103/PhysRevD.76.013006 [arXiv:0704.1596 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.76.013006 2007
-
[25]
S. Zhou, “Update on Two-Zero Textures of the Majorana Neutrino Mass Matrix in Light of Recent T2K, Super-Kamiokande and NOvA Data,” Chin. Phys. C40, 033102 (2016) doi:10.1088/1674-1137/40/3/033102 [arXiv:1509.05300 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/1674-1137/40/3/033102 2016
-
[26]
Texture Zeros and Majorana Phases of the Neutrino Mass Ma- trix,
H. Fritzsch and Z. z. Xing, “Texture Zeros and Majorana Phases of the Neutrino Mass Ma- trix,” Prog. Part. Nucl. Phys.45, 1 (2000) doi:10.1016/S0146-6410(00)00102-2 [arXiv:hep- ph/9912358]
-
[27]
A discrete symmetry group for maximal atmospheric neutrino mixing
W. Grimus and L. Lavoura, “A Discrete Symmetry Group for Maximal Atmospheric Neutrino Mixing,” Phys. Lett. B572, 189 (2003) doi:10.1016/j.physletb.2003.08.032 [arXiv:hep-ph/0305046]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/j.physletb.2003.08.032 2003
-
[28]
Texture Zeros and Weak Basis Transformations
G. C. Branco, D. Emmanuel-Costa and R. Gonzalez Felipe, “Texture Zeros and Weak Basis Transformations,” Phys. Lett. B477, 147 (2000) doi:10.1016/S0370-2693(00)00197- 0 [arXiv:hep-ph/9911418]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/s0370-2693(00)00197- 2000
-
[29]
Discrete Flavor Symmetries and Models of Neutrino Mixing
G. Altarelli and F. Feruglio, “Discrete Flavor Symmetries and Models of Neutrino Mixing,” Rev. Mod. Phys.82, 2701 (2010) doi:10.1103/RevModPhys.82.2701 [arXiv:1002.0211 [hep- ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/revmodphys.82.2701 2010
-
[30]
Neutrino Mass and Mixing with Discrete Symmetry
S. F. King and C. Luhn, “Neutrino Mass and Mixing with Discrete Symmetry,” Rept. Prog. Phys.76, 056201 (2013) doi:10.1088/0034-4885/76/5/056201 [arXiv:1301.1340 [hep-ph]]. 19
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/0034-4885/76/5/056201 2013
-
[31]
Baryogenesis without Grand Unification,
M. Fukugita and T. Yanagida, “Baryogenesis without Grand Unification,” Phys. Lett. B 174, 45 (1986)
work page 1986
-
[32]
S. Davidson, E. Nardi and Y. Nir, “Leptogenesis,” Phys. Rept.466, 105 (2008)
work page 2008
-
[33]
W. Buchmuller, P. Di Bari and M. Plumacher, “Leptogenesis for Pedestrians,” Annals Phys.315, 305 (2005)
work page 2005
-
[34]
The Importance of Flavor in Leptogenesis,
E. Nardi et al., “The Importance of Flavor in Leptogenesis,” JHEP0601, 164 (2006)
work page 2006
-
[35]
Flavour Matters in Leptogenesis,
A. Abada et al., “Flavour Matters in Leptogenesis,” JHEP0609, 010 (2006)
work page 2006
-
[36]
CP Violation and Baryogenesis due to Heavy Majorana Neutrinos,
A. Pilaftsis, “CP Violation and Baryogenesis due to Heavy Majorana Neutrinos,” Phys. Rev. D56, 5431 (1997)
work page 1997
-
[37]
A. Pilaftsis and T. E. J. Underwood, “Resonant Leptogenesis,” Nucl. Phys. B692, 303 (2004)
work page 2004
-
[38]
Resonant Leptogenesis in the Minimal Seesaw Model,
P. S. B. Dev et al., “Resonant Leptogenesis in the Minimal Seesaw Model,” Phys. Rev. D 86, 113001 (2012)
work page 2012
-
[39]
Leptogenesis from Scalar Triplet Decays,
T. Hambye et al., “Leptogenesis from Scalar Triplet Decays,” Nucl. Phys. B695, 169 (2004)
work page 2004
-
[40]
Neutrino Masses and Leptogenesis with Heavy Higgs Triplets,
E. Ma and U. Sarkar, “Neutrino Masses and Leptogenesis with Heavy Higgs Triplets,” Phys. Rev. Lett.80, 5716 (1998)
work page 1998
-
[41]
Supersymmetric Seesaw without Singlet Neutrinos: Neutrino Masses and Lep- togenesis,
A. Rossi, “Supersymmetric Seesaw without Singlet Neutrinos: Neutrino Masses and Lep- togenesis,” Phys. Rev. D66, 075003 (2002)
work page 2002
-
[42]
Non-resonant Higgs pair production in the $b\bar{b}b\bar{b}$ final state at the LHC
A. Chaudhuri, W. Grimus and B. Mukhopadhyaya, “Doubly Charged Scalar De- cays in a Type II Seesaw Scenario with Two Higgs Triplets,” JHEP02, 060 (2015) doi:10.1007/JHEP02(2015)060 [arXiv:1410.2794 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep02(2015)060 2015
-
[43]
Searching for the Tracy-Widom distribution in nonequilibrium processes
A. Chaudhuri and B. Mukhopadhyaya, “CP-violating Phase in a Two Higgs Triplet Sce- nario: Some Phenomenological Implications,” Phys. Rev. D93, no.9, 093003 (2016) doi:10.1103/PhysRevD.93.093003 [arXiv:1512.06292 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.93.093003 2016
-
[44]
A. Chaudhuri, “Resonant Leptogenesis in a Two-Triplet Type-II Seesaw: A Dynamical Origin of Suppressed Lepton Flavor Violation,” arXiv:2604.11002 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv
-
[45]
Inverse Beta Processes and Nonconservation of Lepton Charge,
B. Pontecorvo, “Inverse Beta Processes and Nonconservation of Lepton Charge,” Sov. Phys. JETP7, 172 (1958)
work page 1958
-
[46]
Remarks on the Unified Model of Elementary Particles,
Z. Maki, M. Nakagawa and S. Sakata, “Remarks on the Unified Model of Elementary Particles,” Prog. Theor. Phys.28, 870 (1962)
work page 1962
-
[47]
R. L. Workman et al. [Particle Data Group], “Review of Particle Physics,” Prog. Theor. Exp. Phys. 2022, 083C01 (2022)
work page 2022
-
[48]
The Fate of Hints: Updated Global Analysis of Three-Flavor Neutrino Oscillations,
I. Esteban et al., “The Fate of Hints: Updated Global Analysis of Three-Flavor Neutrino Oscillations,” JHEP2009, 178 (2020)
work page 2020
-
[49]
Flavor Effects on Leptogenesis Predictions,
S. Blanchet and P. Di Bari, “Flavor Effects on Leptogenesis Predictions,” JCAP0703, 018 (2007)
work page 2007
-
[50]
Flavour Effects in Leptogenesis,
M. Beneke et al., “Flavour Effects in Leptogenesis,” Nucl. Phys. B843, 177 (2011). 20
work page 2011
-
[51]
Flavored Quantum Boltzmann Equations
V. Cirigliano, C. Lee, M. J. Ramsey-Musolf and S. Tulin, “Flavored Leptogenesis, Quantum Coherence, and the CP Asymmetry,” Phys. Rev. D81, 103503 (2010) doi:10.1103/PhysRevD.81.103503 [arXiv:0912.3523 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.81.103503 2010
-
[52]
M. Garny, A. Hohenegger, A. Kartavtsev and M. Lindner, “Quantum Corrections to Leptogenesis from the Gradient Expansion,” Phys. Rev. D80, 125027 (2009) doi:10.1103/PhysRevD.80.125027 [arXiv:0909.1559 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.80.125027 2009
-
[53]
The view of AGN-host alignment via reflection spectroscopy
A. Kartavtsev, P. Millington and H. Vogel, “Leptogenesis in the Quantum Regime,” JHEP 1606, 066 (2016) doi:10.1007/JHEP06(2016)066 [arXiv:1601.03090 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep06(2016)066 2016
-
[54]
Reconciling leptogenesis with observable mu --> e gamma rates
S. Blanchet, T. Hambye and F. X. Josse-Michaux, “Reconciling Leptogenesis with Observableµ→eγRates,” JHEP1004, 023 (2010) doi:10.1007/JHEP04(2010)023 [arXiv:0912.3153 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep04(2010)023 2010
-
[55]
Lepton Flavour Violation and theta(13) in Minimal Resonant Leptogenesis
F. F. Deppisch and A. Pilaftsis, “Lepton Flavour Violation and Resonant Leptogenesis,” Phys. Rev. D83, 076007 (2011) doi:10.1103/PhysRevD.83.076007 [arXiv:1012.1834 [hep- ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.83.076007 2011
-
[56]
E. W. Kolb and M. S. Turner, “The Early Universe,” Front. Phys.69, 1 (1990)
work page 1990
-
[57]
Towards a Complete Theory of Thermal Leptogenesis,
G. F. Giudice et al., “Towards a Complete Theory of Thermal Leptogenesis,” Nucl. Phys. B685, 89 (2004)
work page 2004
-
[58]
On the Anomalous Electroweak Baryon Number Nonconservation in the Early Universe,
V. A. Kuzmin, V. A. Rubakov and M. E. Shaposhnikov, “On the Anomalous Electroweak Baryon Number Nonconservation in the Early Universe,” Phys. Lett. B155, 36 (1985) doi:10.1016/0370-2693(85)91028-7
-
[59]
Fusion rules and modular transformations in 2D conformal field theory
S. Y. Khlebnikov and M. E. Shaposhnikov, “The Statistical Theory of Anomalous Fermion Number Nonconservation,” Nucl. Phys. B308, 885 (1988) doi:10.1016/0550- 3213(88)90133-2
-
[60]
Cosmological Baryon and Lepton Number in the Presence of Electroweak Fermion Number Violation,
J. A. Harvey and M. S. Turner, “Cosmological Baryon and Lepton Number in the Presence of Electroweak Fermion Number Violation,” Phys. Rev. D42, 3344 (1990) doi:10.1103/PhysRevD.42.3344
-
[61]
Baryon and lepton number violation rates across the electroweak crossover
Y. Burnier, M. Laine and M. Shaposhnikov, “Baryon and Lepton Number Violation Rates across the Electroweak Crossover,” JCAP0602, 007 (2006) doi:10.1088/1475- 7516/2006/02/007 [arXiv:hep-ph/0511246]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/1475- 2006
-
[62]
Sphalerons, Small Fluctuations and Baryon Number Violation in Electroweak Theory,
P. Arnold and L. McLerran, “Sphalerons, Small Fluctuations and Baryon Number Violation in Electroweak Theory,” Phys. Rev. D36, 581 (1987) doi:10.1103/PhysRevD.36.581
-
[63]
Baryon Asymmetry of the Universe in Standard Electroweak The- ory,
M. E. Shaposhnikov, “Baryon Asymmetry of the Universe in Standard Electroweak The- ory,” Nucl. Phys. B287, 757 (1987) doi:10.1016/0550-3213(87)90127-1. 21
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