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Minimal A4 type-II seesaw realization of testable neutrino mass sum rules

Salvador Centelles Chuliá1,* and Ranjeet Kumar2,3,†

  • *Contact author: salcen@ific.uv.es
  • †Contact author: kumarranjeet.drk@gmail.com

Phys. Rev. D 113, 055023 – Published 13 March, 2026

DOI: https://doi.org/10.1103/ndvc-1vpl

Abstract

We propose a flavor model based on an A4 symmetry combined with a type-II seesaw mechanism for neutrino mass generation. The resulting neutrino mass matrix obeys a sum rule that, together with the measured mass-squared differences, fully determines the absolute neutrino mass spectrum. The constrained flavor structure yields correlated predictions for lepton mixing parameters, leads to inverted ordering after imposing mixing constraints, restricts the Majorana phases and implies a neutrinoless double beta decay rate close to its maximal value for inverted ordering. In the charged lepton sector an approximate triality symmetry arises in the seesaw limit, suppressing muon flavor-violating processes and allowing only specific τ decay channels. The model provides a tightly constrained and experimentally testable framework linking neutrino masses, lepton mixing, and lepton-number-violating observables.

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References (83)

  1. K. S. Babu and R. N. Mohapatra, Permutation symmetry and the origin of fermion mass hierarchy, Phys. Rev. Lett. 64, 2747 (1990).
  2. P. H. Frampton and T. W. Kephart, Simple nonabelian finite flavor groups and fermion masses, Int. J. Mod. Phys. A 10, 4689 (1995).
  3. J. Kubo, A. Mondragon, M. Mondragon, and E. Rodriguez-Jauregui, The flavor symmetry, Prog. Theor. Phys. 109, 795 (2003); 114, 287(E) (2005).
  4. G. Altarelli and F. Feruglio, Discrete flavor symmetries and models of neutrino mixing, Rev. Mod. Phys. 82, 2701 (2010).
  5. S. Morisi and J. W. F. Valle, Neutrino masses and mixing: A flavour symmetry roadmap, Fortschr. Phys. 61, 466 (2013).
  6. F. Feruglio and A. Romanino, Lepton flavor symmetries, Rev. Mod. Phys. 93, 015007 (2021).
  7. P. B. Denton and J. Gehrlein, Survey of neutrino flavor predictions and the neutrinoless double beta decay funnel, Phys. Rev. D 109, 055028 (2024).
  8. G.-J. Ding and J. W. F. Valle, The symmetry approach to quark and lepton masses and mixing, Phys. Rep. 1109, 1 (2025).
  9. H. Ishimori et al., Non-Abelian discrete symmetries in particle physics, Prog. Theor. Phys. Suppl. 183, 1 (2010).
  10. K. Babu, E. Ma, and J. W. F. Valle, Underlying A4 symmetry for the neutrino mass matrix and the quark mixing matrix, Phys. Lett. B 552, 207 (2003).
  11. S.-L. Chen, M. Frigerio, and E. Ma, Hybrid seesaw neutrino masses with A4 family symmetry, Nucl. Phys. B724, 423 (2005).
  12. G. Altarelli and F. Feruglio, Tri-bimaximal neutrino mixing, A4 and the modular symmetry, Nucl. Phys. B741, 215 (2006).
  13. A. E. Carcamo Hernandez, I. de Medeiros Varzielas, S. G. Kovalenko, H. Päs, and I. Schmidt, Lepton masses and mixings in an A4 multi-Higgs model with a radiative seesaw mechanism, Phys. Rev. D 88, 076014 (2013).
  14. A. E. Cárcamo Hernández and R. Martinez, A predictive 3−3−1 model with A4 flavor symmetry, Nucl. Phys. B905, 337 (2016).
  15. D. Borah and B. Karmakar, A4 flavour model for Dirac neutrinos: Type I and inverse seesaw, Phys. Lett. B 780, 461 (2018).
  16. A. E. Cárcamo Hernández and H. N. Long, A highly predictive A4 flavour 3-3-1 model with radiative inverse seesaw mechanism, J. Phys. G 45, 045001 (2018).
  17. S. Centelles Chuliá, R. Srivastava, and J. W. F. Valle, Generalized Bottom-Tau unification, neutrino oscillations and dark matter: Predictions from a lepton quarticity flavor approach, Phys. Lett. B 773, 26 (2017).
  18. D. Borah and B. Karmakar, Linear seesaw for Dirac neutrinos with A4 flavour symmetry, Phys. Lett. B 789, 59 (2019).
  19. G.-J. Ding, J.-N. Lu, and J. W. F. Valle, Trimaximal neutrino mixing from scotogenic A4 family symmetry, Phys. Lett. B 815, 136122 (2021).
  20. M. R. Devi and K. Bora, Exploring the feasibility of the charged lepton flavor violating decay μ→e+γ in inverse and linear seesaw mechanisms with A4 flavor symmetry, Mod. Phys. Lett. A 37, 2250206 (2022).
  21. K. Bora and M. R. Devi, Exploring dynamics of A4 flavour symmetry using low scale seesaw mechanisms, Phys. Part. Nucl. Lett. 19, 642 (2022).
  22. M. Ricky Devi and K. Bora, Linking resonant leptogenesis with dynamics of the inverse seesaw theory with A4 flavor symmetry, arXiv:2304.13546.
  23. R. Kumar, P. Mishra, M. K. Behera, R. Mohanta, and R. Srivastava, Predictions from scoto-seesaw with A4 modular symmetry, Phys. Lett. B 853, 138635 (2024).
  24. S. Mahapatra, S. K. Sahoo, N. Sahu, and V. S. Thounaojam, Self-interacting dark matter and Dirac neutrinos via lepton quarticity, Phys. Rev. D 109, 055036 (2024).
  25. L. Singh, M. Kashav, and S. Verma, Minimal type-I Dirac seesaw and leptogenesis under A4 modular invariance, Nucl. Phys. B 1007, 116666 (2024).
  26. R. Kumar, N. Nath, and R. Srivastava, Cutting the scotogenic loop: Adding flavor to dark matter, J. High Energy Phys. 12 (2024) 036.
  27. T. Nomura and H. Okada, Type-II seesaw of a non-holomorphic modular A4 symmetry, Phys. Lett. B 868, 139763 (2025).
  28. A. Palavrić, Discrete leptonic flavor symmetries: UV mediators and phenomenology, Phys. Rev. D 110, 115025 (2024).
  29. G. Pathak, P. Das, and M. K. Das, Neutrino mass genesis in scoto-inverse seesaw with modular A4, Eur. Phys. J. C 85, 569 (2025).
  30. S. T. Goswami and S. Roy, Permuted charged lepton correction in the framework of Dirac seesaw, Nucl. Phys. B1022, 117275 (2026).
  31. A. Moreno-Sánchez and A. Palavrić, Leptonic flavor from a modular A4 symmetry: UV mediators and SMEFT realizations, Phys. Rev. D 112, 075002 (2025).
  32. R. Kumar, N. Nath, R. Srivastava, and S. Yadav, Dirac scoto inverse-seesaw from A4 flavor symmetry, J. High Energy Phys. 10 (2025) 088.
  33. R. Kumar, H. K. Prajapati, R. Srivastava, and S. Yadav, Flavor imprints on novel low mass dark matter, J. High Energy Phys. 11 (2025) 094.
  34. E. Ma and G. Rajasekaran, Softly broken A4 symmetry for nearly degenerate neutrino masses, Phys. Rev. D 64, 113012 (2001).
  35. E. Ma, Quark and lepton flavor triality, Phys. Rev. D 82, 037301 (2010).
  36. Q.-H. Cao, A. Damanik, E. Ma, and D. Wegman, Probing lepton flavor triality with Higgs boson decay, Phys. Rev. D 83, 093012 (2011).
  37. L. Calibbi, C. Hagedorn, M. A. Schmidt, and J. Vandeleur, Selection rules for charged lepton flavour violating processes from residual flavour groups, Phys. Rev. D 112, 075031 (2025).
  38. I. de Medeiros Varzielas, M.-S. Liu, A. Sengupta, and J. Talbert, Residual symmetries and scalar multiplet vacuum alignment in non-Abelian flavour models, arXiv:2512.19789.
  39. T. Kajita, Nobel lecture: Discovery of atmospheric neutrino oscillations, Rev. Mod. Phys. 88, 030501 (2016).
  40. A. B. McDonald, Nobel lecture: The Sudbury Neutrino Observatory: Observation of flavor change for solar neutrinos, Rev. Mod. Phys. 88, 030502 (2016).
  41. J. Schechter and J. W. F. Valle, Neutrino masses in SU(2)×U(1) theories, Phys. Rev. D 22, 2227 (1980).
  42. M. Magg and C. Wetterich, Neutrino mass problem and gauge hierarchy, Phys. Lett. 94B, 61 (1980).
  43. T. P. Cheng and L.-F. Li, Neutrino masses, mixings and oscillations in SU(2)×U(1) models of electroweak interactions, Phys. Rev. D 22, 2860 (1980).
  44. R. N. Mohapatra and G. Senjanovic, Neutrino masses and mixings in gauge models with spontaneous parity violation, Phys. Rev. D 23, 165 (1981).
  45. E. Ma and U. Sarkar, Neutrino masses and leptogenesis with heavy Higgs triplets, Phys. Rev. Lett. 80, 5716 (1998).
  46. S. Antusch and S. F. King, Type II leptogenesis and the neutrino mass scale, Phys. Lett. B 597, 199 (2004).
  47. S. Antusch, Flavour-dependent type II leptogenesis, Phys. Rev. D 76, 023512 (2007).
  48. N. D. Barrie, C. Han, and H. Murayama, Affleck-Dine leptogenesis from Higgs inflation, Phys. Rev. Lett. 128, 141801 (2022).
  49. N. D. Barrie, C. Han, and H. Murayama, Type II seesaw leptogenesis, J. High Energy Phys. 05 (2022) 160.
  50. M. Berbig, Type II seesaw leptogenesis in a Majoron background, arXiv:2506.23290.
  51. L. Lavoura, General formulae for f1→f2γ, Eur. Phys. J. C 29, 191 (2003).
  52. D. N. Dinh, A. Ibarra, E. Molinaro, and S. T. Petcov, The μ−e conversion in nuclei, μ→eγ,μ→3e decays and TeV scale see-saw scenarios of neutrino mass generation, J. High Energy Phys. 08 (2012) 125; 09 (2013) 023(E).
  53. N. D. Barrie and S. T. Petcov, Lepton flavour violation tests of type II seesaw leptogenesis, J. High Energy Phys. 01 (2023) 001.
  54. S. Mandal, O. G. Miranda, G. Sanchez Garcia, J. W. F. Valle, and X.-J. Xu, Toward deconstructing the simplest seesaw mechanism, Phys. Rev. D 105, 095020 (2022).
  55. J. Barry and W. Rodejohann, Neutrino mass sum-rules in flavor symmetry models, Nucl. Phys. B842, 33 (2011).
  56. S. F. King, A. Merle, and A. J. Stuart, The power of neutrino mass sum rules for neutrinoless double beta decay experiments, J. High Energy Phys. 12 (2013) 005.
  57. J. Gehrlein, A. Merle, and M. Spinrath, Predictivity of neutrino mass sum rules, Phys. Rev. D 94, 093003 (2016).
  58. J. Gehrlein and M. Spinrath, Leptonic sum rules from flavour models with modular symmetries, J. High Energy Phys. 03 (2021) 177.
  59. S. Chuliá Centelles, R. Cepedello, and O. Medina, Absolute neutrino mass scale and dark matter stability from flavour symmetry, J. High Energy Phys. 10 (2022) 080.
  60. S. Centelles Chuliá, R. Kumar, O. Popov, and R. Srivastava, Neutrino mass sum rules from modular A4 symmetry, Phys. Rev. D 109, 035016 (2024).
  61. W. Rodejohann and J. W. F. Valle, Symmetrical parametrizations of the lepton mixing matrix, Phys. Rev. D 84, 073011 (2011).
  62. M. P. Bento, J. P. Silva, and A. Trautner, The basis invariant flavor puzzle, J. High Energy Phys. 01 (2024) 024.
  63. P. F. de Salas, D. V. Forero, S. Gariazzo, P. Martínez-Miravé, O. Mena, C. A. Ternes, M. Tórtola, and J. W. F. Valle, 2020 global reassessment of the neutrino oscillation picture, J. High Energy Phys. 02 (2021) 071.
  64. N. Aghanim et al. (Planck Collaboration), Planck 2018 results. VI. Cosmological parameters, Astron. Astrophys. 641, A6 (2020); 652, C4(E) (2021).
  65. E. Camphuis et al. (SPT-3G Collaboration), SPT-3G D1: CMB temperature and polarization power spectra and cosmology from 2019 and 2020 observations of the SPT-3G main field, arXiv:2506.20707.
  66. L. Amendola et al., Cosmology and fundamental physics with the Euclid satellite, Living Rev. Relativity 21, 2 (2018).
  67. T. Bertólez-Martínez, I. Esteban, R. Hajjar, O. Mena, and J. Salvado, Origin of cosmological neutrino mass bounds: Background versus perturbations, J. Cosmol. Astropart. Phys. 06 (2025) 058.
  68. D. Naredo-Tuero, M. Escudero, E. Fernández-Martínez, X. Marcano, and V. Poulin, Critical look at the cosmological neutrino mass bound, Phys. Rev. D 110, 123537 (2024).
  69. M. Aker et al. (KATRIN Collaboration), Direct neutrino-mass measurement based on 259 days of KATRIN data, Science 388, adq9592 (2025).
  70. A. Ashtari Esfahani et al. (Project 8 Collaboration), Tritium beta spectrum measurement and neutrino mass limit from cyclotron radiation emission spectroscopy, Phys. Rev. Lett. 131, 102502 (2023).
  71. A. Ashtari Esfahani et al. (Project 8 Collaboration), Antenna arrays for neutrino mass measurements with cyclotron radiation emission spectroscopy, Phys. Rev. C 112, 045506 (2025).
  72. A. A. Esfahani et al. (Project 8 Collaboration), The project 8 neutrino mass experiment, in Snowmass 2021 (2022), arXiv:2203.07349.
  73. A. N. Khan, H. Nunokawa, and S. J. Parke, Why matter effects matter for JUNO, Phys. Lett. B 803, 135354 (2020).
  74. A. Abusleme et al. (JUNO Collaboration), First measurement of reactor neutrino oscillations at JUNO, arXiv:2511.14593.
  75. M. A. Acero et al. (NOvA Collaboration), Improved measurement of neutrino oscillation parameters by the NOvA experiment, Phys. Rev. D 106, 032004 (2022).
  76. K. Abe et al. (T2K Collaboration), Measurements of neutrino oscillation parameters from the T2K experiment using 3.6×1021 protons on target, Eur. Phys. J. C 83, 782 (2023).
  77. B. Abi et al. (DUNE Collaboration), Deep underground neutrino experiment (DUNE), far detector technical design report, volume II: DUNE physics, arXiv:2002.03005.
  78. K. Abe et al. (Hyper-Kamiokande Collaboration), Hyper-Kamiokande design report, arXiv:1805.04163.
  79. S. Abe et al. (KamLAND-Zen Collaboration), Search for Majorana neutrinos with the complete KamLAND-Zen dataset, Phys. Rev. Lett. 135, 262501 (2025).
  80. J. Nakane, New detector development and performance evaluation for KamLAND2-Zen experiment, Nucl. Instrum. Methods Phys. Res., Sect. A 1081, 170850 (2026).
  81. S. Navas et al. (Particle Data Group), Review of particle physics, Phys. Rev. D 110, 030001 (2024).
  82. N. Buskin and I. P. Ivanov, Bounded-from-below conditions for A4-symmetric 3HDM, J. Phys. A 54, 325401 (2021).
  83. M. P. Bento, H. E. Haber, J. C. Romão, and J. P. Silva, Multi-Higgs doublet models: The Higgs-fermion couplings and their sum rules, J. High Energy Phys. 10 (2018) 143.

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