Pith. sign in

REVIEW 192 references

Phenomenological Aspects of Models with Low Scale Seesaw

Not yet reviewed by Pith; the record is open.

This paper has not been read by Pith yet. Machine review is queued; the pith claim, tier, and objections will appear here once it completes.

SPECIMEN: schema-true, not a live event

T0 review · schema-true

One-sentence machine reading of the paper's core claim.

pith:XXXXXXXX · record.json · timestamp

arxiv 2412.07695 v1 pith:BRYPY2HH submitted 2024-12-10 hep-ph

classification hep-ph
keywords beenphenomenologicalseesawtheoriesaspectsconsistentexperimentalfermion
topics Dark Matter
open problems Dark Matter
verification ladder T0 review T1 audit T2 compute T3 formal
0 comments
abstract

Various phenomenological consequences of seesaw theories for the generation of the fermion mass hierarchy of the Standard Model have been analyzed, with an emphasis on models in which the light-active neutrino masses are derived from low-scale seesaw mechanisms. In particular, fermion masses and lepton flavor-violating decay processes, the flavor-changing neutral current, have been studied, and the implications of these theories for the observed dark matter relic density in the Universe have been determined. From the analysis of these phenomenological aspects, it was possible to determine the allowed parameter spaces of these theories and to obtain a parameter fit consistent with the currently measured experimental values. In this way, correlations between the different observables of the fermionic sector could be obtained, where all values were within the experimental ranges at $3\sigma$. Predictions for new physics consistent with cosmological limits were also obtained.

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

192 extracted references · 23 canonical work pages

  1. [1]

    Results from one thousand days of real time directional solar neutrino data,

    Kamiokande-II Collaboration, K. S. Hirata et al., “Results from one thousand days of real time directional solar neutrino data,” Phys. Rev. Lett. 65 (1990) 1297–1300

  2. [2]

    Search for neutrinos from the sun,

    R. Davis, Jr., D. S. Harmer, and K. C. Hoffman, “Search for neutrinos from the sun,” Phys. Rev. Lett. 20 (1968) 1205–1209

  3. [3]

    Evidence for oscillation of atmospheric neutrinos,

    Super-Kamiokande Collaboration, Y . Fukudaet al., “Evidence for oscillation of atmospheric neutrinos,” Phys. Rev. Lett. 81 (1998) 1562–1567, arXiv:hep-ex/9807003

  4. [4]

    Observation of a small atmospheric muon-neutrino / electron-neutrino ratio in Kamiokande,

    Kamiokande-II Collaboration, K. S. Hirata et al., “Observation of a small atmospheric muon-neutrino / electron-neutrino ratio in Kamiokande,” Phys. Lett. B 280 (1992) 146–152

  5. [5]

    Solar B-8 and hep neutrino measurements from 1258 days of Super-Kamiokande data,

    Super-Kamiokande Collaboration, S. Fukuda et al., “Solar B-8 and hep neutrino measurements from 1258 days of Super-Kamiokande data,” Phys. Rev. Lett. 86 (2001) 5651–5655, arXiv:hep-ex/0103032

  6. [6]

    First results from KamLAND: Evidence for reactor anti-neutrino disappearance,

    KamLAND Collaboration, K. Eguchi et al., “First results from KamLAND: Evidence for reactor anti-neutrino disappearance,” Phys. Rev. Lett. 90 (2003) 021802, arXiv:hep-ex/0212021

  7. [7]

    Precision Measurement of Neutrino Oscillation Parameters with KamLAND,

    KamLAND Collaboration, S. Abe et al., “Precision Measurement of Neutrino Oscillation Parameters with KamLAND,” Phys. Rev. Lett. 100 (2008) 221803, arXiv:0801.4589 [hep-ex]

  8. [8]

    Precise Measurement of the Neutrino Mixing Parameter θ23 from Muon Neutrino Disappearance in an Off-Axis Beam,

    T2K Collaboration, K. Abe et al., “Precise Measurement of the Neutrino Mixing Parameter θ23 from Muon Neutrino Disappearance in an Off-Axis Beam,” Phys. Rev. Lett. 112 no. 18, (2014) 181801, arXiv:1403.1532 [hep-ex]

Show all 192 references
  1. [9]

    Observation of Reactor Electron Antineutrino Disappearance in the RENO Experiment,

    RENO Collaboration, J. K. Ahn et al., “Observation of Reactor Electron Antineutrino Disappearance in the RENO Experiment,” Phys. Rev. Lett. 108 (2012) 191802, arXiv:1204.0626 [hep-ex]

  2. [10]

    2020 global reassessment of the neutrino oscillation picture,

    P. F. de Salas, D. V . Forero, S. Gariazzo, P. Mart´ınez-Mirav´e, O. Mena, C. A. Ternes, M. T´ortola, and J. W. F. Valle, “2020 global reassessment of the neutrino oscillation picture,”JHEP 02 (2021) 071, arXiv:2006.11237 [hep-ph]

  3. [11]

    Teor ´ıa cu´antica de campos,

    J. I. Illana, “Teor ´ıa cu´antica de campos,” 2017

  4. [12]

    Maggiore, A modern introduction to quantum field theory, vol

    M. Maggiore, A modern introduction to quantum field theory, vol. 12. Oxford university press, 2005

  5. [13]

    M. E. Peskin, An introduction to quantum field theory. CRC Press, 2018

  6. [14]

    The Standard model of electroweak interactions,

    A. Pich, “The Standard model of electroweak interactions,” in The Standard model of electroweak interactions, pp. 1–49. 2008. arXiv:0705.4264 [hep-ph] . http://doc.cern.ch/yellowrep/2007/2007-005/cern-2007-005.pdf . [,1(2007)]

  7. [15]

    M. D. Schwartz, Quantum field theory and the standard model. Cambridge University Press, 2014

  8. [16]

    Georgi, Lie algebras in particle physics: from isospin to unified theories

    H. Georgi, Lie algebras in particle physics: from isospin to unified theories. CRC Press, 2018

  9. [17]

    Field theories with ≪superconductor≫ solutions,

    J. Goldstone, “Field theories with ≪superconductor≫ solutions,” Il Nuovo Cimento (1955-1965) 19 no. 1, (1961) 154–164. 90 Bibliography 91

  10. [18]

    Broken symmetry and the mass of gauge vector mesons,

    F. Englert and R. Brout, “Broken symmetry and the mass of gauge vector mesons,” Physical Review Letters 13 no. 9, (1964) 321

  11. [19]

    Langacker, The standard model and beyond

    P. Langacker, The standard model and beyond. CRC press, 2017

  12. [20]

    El modelo est ´andar y su fenomenolog´ıa,

    J. I. Illana, “El modelo est ´andar y su fenomenolog´ıa,” 2007

  13. [21]

    Flavour Dynamics and Violations of the CP Symmetry,

    A. Pich, “Flavour Dynamics and Violations of the CP Symmetry,” CERN YellowRep. School Proc. 4 (2018) 65, arXiv:1805.08597 [hep-ph]

  14. [22]

    Introduction to flavour physics,

    J. Zupan, “Introduction to flavour physics,” in 2018 European School of High-Energy Physics (ESHEP2018) Maratea, Italy, June 20-July 3, 2018. 2019. arXiv:1903.05062 [hep-ph]

  15. [23]

    The hierarchy problem of the electroweak standard model revisited,

    F. Jegerlehner, “The hierarchy problem of the electroweak standard model revisited,” arXiv preprint arXiv:1305.6652 (2013)

  16. [24]

    New solutions to the hierarchy problem,

    G. Burdman, “New solutions to the hierarchy problem,” Brazilian journal of physics 37 (2007) 506–513

  17. [25]

    Quark Mass Hierarchy and Flavor Mixing Puzzles,

    Z.-z. Xing, “Quark Mass Hierarchy and Flavor Mixing Puzzles,” Int. J. Mod. Phys. A 29 (2014) 1430067, arXiv:1411.2713 [hep-ph]

  18. [26]

    Pieces of the Flavour Puzzle,

    F. Feruglio, “Pieces of the Flavour Puzzle,” Eur. Phys. J. C 75 no. 8, (2015) 373, arXiv:1503.04071 [hep-ph]

  19. [27]

    Mass and flavor mixing schemes of quarks and leptons,

    H. Fritzsch and Z.-z. Xing, “Mass and flavor mixing schemes of quarks and leptons,” Prog. Part. Nucl. Phys. 45 (2000) 1–81, arXiv:hep-ph/9912358

  20. [28]

    Mesonium and antimesonium,

    B. Pontecorvo, “Mesonium and antimesonium,” Zhur. Eksptl’. i Teoret. Fiz. 33 (8, 1957) . https://www.osti.gov/biblio/4343073

  21. [29]

    Direct evidence for neutrino flavor transformation from neutral current interactions in the Sudbury Neutrino Observatory,

    SNO Collaboration, Q. R. Ahmad et al., “Direct evidence for neutrino flavor transformation from neutral current interactions in the Sudbury Neutrino Observatory,” Phys. Rev. Lett. 89 (2002) 011301, arXiv:nucl-ex/0204008

  22. [30]

    Neutrino Mass and Mixing: from Theory to Experiment,

    S. F. King, A. Merle, S. Morisi, Y . Shimizu, and M. Tanimoto, “Neutrino Mass and Mixing: from Theory to Experiment,” New J. Phys. 16 (2014) 045018, arXiv:1402.4271 [hep-ph]

  23. [31]

    Rotation of the Andromeda Nebula from a Spectroscopic Survey of Emission Regions,

    V . C. Rubin and W. K. Ford, Jr., “Rotation of the Andromeda Nebula from a Spectroscopic Survey of Emission Regions,” Astrophys. J. 159 (1970) 379–403

  24. [32]

    Letter to l. meitner and her colleagues,

    W. Pauli, “Letter to l. meitner and her colleagues,” Phys. Today 9 (1930) 23

  25. [33]

    Detection of the free neutrino,

    F. Reines and C. L. Cowan, “Detection of the free neutrino,” Phys. Rev. 92 (1953) 830–831

  26. [34]

    Mesonium and anti-mesonium,

    B. Pontecorvo, “Mesonium and anti-mesonium,” Sov. Phys. JETP 6 (1957) 429

  27. [35]

    Inverse beta processes and nonconservation of lepton charge,

    B. Pontecorvo, “Inverse beta processes and nonconservation of lepton charge,” Zh. Eksp. Teor.Fiz. 34 (1957) 247

  28. [36]

    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 (1962) 870–880

  29. [37]

    Giunti and C

    C. Giunti and C. W. Kim, Fundamentals of neutrino physics and astrophysics. Oxford university press, 2007

  30. [38]

    Planck 2018 results. VI. Cosmological parameters,

    Planck Collaboration, N. Aghanim et al., “Planck 2018 results. VI. Cosmological parameters,” Astron. Astrophys. 641 (2020) A6, arXiv:1807.06209 [astro-ph.CO] . [Erratum: Astron.Astrophys. 652, C4 (2021)]

  31. [39]

    Search for Majorana Neutrinos with the Complete KamLAND-Zen Dataset,

    KamLAND-Zen Collaboration, S. Abe et al., “Search for Majorana Neutrinos with the Complete KamLAND-Zen Dataset,” arXiv:2406.11438 [hep-ex] . 92 CHAPTER 7. BIBLIOGRAPHY

  32. [40]

    Baryon and Lepton Nonconserving Processes,

    S. Weinberg, “Baryon and Lepton Nonconserving Processes,” Phys. Rev. Lett. 43 (1979) 1566–1570

  33. [41]

    Neutrino Mass and Spontaneous Parity Nonconservation,

    R. N. Mohapatra and G. Senjanovic, “Neutrino Mass and Spontaneous Parity Nonconservation,” Phys. Rev. Lett. 44 (1980) 912

  34. [42]

    Mechanism for Understanding Small Neutrino Mass in Superstring Theories,

    R. N. Mohapatra, “Mechanism for Understanding Small Neutrino Mass in Superstring Theories,” Phys. Rev. Lett. 56 (1986) 561–563

  35. [43]

    Neutrino masses in a 331 model with right-handed neutrinos without doubly charged Higgs bosons via inverse and double seesaw mechanisms,

    M. E. Catano, R. Martinez, and F. Ochoa, “Neutrino masses in a 331 model with right-handed neutrinos without doubly charged Higgs bosons via inverse and double seesaw mechanisms,”Phys. Rev. D 86 (2012) 073015, arXiv:1206.1966 [hep-ph]

  36. [44]

    Stability and symmetry breaking in the general two-Higgs-doublet model,

    M. Maniatis, A. von Manteuffel, O. Nachtmann, and F. Nagel, “Stability and symmetry breaking in the general two-Higgs-doublet model,” Eur. Phys. J. C 48 (2006) 805–823, arXiv:hep-ph/0605184

  37. [45]

    Scalar sector of two-Higgs-doublet models: A minireview,

    G. Bhattacharyya and D. Das, “Scalar sector of two-Higgs-doublet models: A minireview,” Pramana 87 no. 3, (2016) 40, arXiv:1507.06424 [hep-ph]

  38. [46]

    Verifiable radiative seesaw mechanism of neutrino mass and dark matter,

    E. Ma, “Verifiable radiative seesaw mechanism of neutrino mass and dark matter,” Phys. Rev. D 73 (2006) 077301, arXiv:hep-ph/0601225

  39. [47]

    Dark Radiative Inverse Seesaw Mechanism,

    A. Ahriche, S. M. Boucenna, and S. Nasri, “Dark Radiative Inverse Seesaw Mechanism,” Phys. Rev. D 93 no. 7, (2016) 075036, arXiv:1601.04336 [hep-ph]

  40. [48]

    Fermion masses and mixings and dark matter constraints in a model with radiative seesaw mechanism,

    N. Bernal, A. E. C ´arcamo Hern´andez, I. de Medeiros Varzielas, and S. Kovalenko, “Fermion masses and mixings and dark matter constraints in a model with radiative seesaw mechanism,”JHEP 05 (2018) 053, arXiv:1712.02792 [hep-ph]

  41. [49]

    Gauged inverse seesaw from dark matter,

    A. Abada, N. Bernal, A. E. C. Hern ´andez, X. Marcano, and G. Piazza, “Gauged inverse seesaw from dark matter,” Eur. Phys. J. C 81 no. 8, (2021) 758, arXiv:2107.02803 [hep-ph]

  42. [50]

    Cosmological and astrophysical signatures of dark matter annihilations into pseudo-Goldstone bosons,

    C. Garcia-Cely, A. Ibarra, and E. Molinaro, “Cosmological and astrophysical signatures of dark matter annihilations into pseudo-Goldstone bosons,” JCAP 02 (2014) 032, arXiv:1312.3578 [hep-ph]

  43. [51]

    Dark matter production from Goldstone boson interactions and implications for direct searches and dark radiation,

    C. Garcia-Cely, A. Ibarra, and E. Molinaro, “Dark matter production from Goldstone boson interactions and implications for direct searches and dark radiation,” JCAP 11 (2013) 061, arXiv:1310.6256 [hep-ph]

  44. [52]

    micrOMEGAs : a code for the calculation of Dark Matter properties in generic models of particle interaction,

    G. Belanger, F. Boudjema, and A. Pukhov, “micrOMEGAs : a code for the calculation of Dark Matter properties in generic models of particle interaction,” in Theoretical Advanced Study Institute in Elementary Particle Physics: The Dark Secrets of the Terascale, pp. 739–790. 2013....

  45. [53]

    A second Higgs from the Higgs portal,

    A. Falkowski, C. Gross, and O. Lebedev, “A second Higgs from the Higgs portal,” JHEP 05 (2015) 057, arXiv:1502.01361 [hep-ph]

  46. [54]

    Dark Matter Search Results from a One Ton-Year Exposure of XENON1T,

    XENON Collaboration, E. Aprile et al., “Dark Matter Search Results from a One Ton-Year Exposure of XENON1T,” Phys. Rev. Lett. 121 no. 11, (2018) 111302, arXiv:1805.12562 [astro-ph.CO]

  47. [55]

    First Dark Matter Search Results from the LUX-ZEPLIN (LZ) Experiment,

    LZ Collaboration, J. Aalbers et al., “First Dark Matter Search Results from the LUX-ZEPLIN (LZ) Experiment,” Phys. Rev. Lett. 131 no. 4, (2023) 041002, arXiv:2207.03764 [hep-ex]

  48. [56]

    Projected WIMP sensitivity of the XENONnT dark matter experiment,

    XENON Collaboration, E. Aprile et al., “Projected WIMP sensitivity of the XENONnT dark matter experiment,” JCAP 11 (2020) 031, arXiv:2007.08796 [physics.ins-det]

  49. [57]

    Status of the Higgs Singlet Extension of the Standard Model after LHC Run 1,

    T. Robens and T. Stefaniak, “Status of the Higgs Singlet Extension of the Standard Model after LHC Run 1,” Eur. Phys. J. C 75 (2015) 104, arXiv:1501.02234 [hep-ph]

  50. [58]

    Handbook of LHC Higgs Cross Sections: 1. Inclusive Observables,

    LHC Higgs Cross Section Working Group Collaboration, S. Dittmaier et al., “Handbook of LHC Higgs Cross Sections: 1. Inclusive Observables,” arXiv:1101.0593 [hep-ph] . Bibliography 93

  51. [59]

    A Precision Search for WIMPs with Charged Cosmic Rays,

    A. Reinert and M. W. Winkler, “A Precision Search for WIMPs with Charged Cosmic Rays,” JCAP 01 (2018) 055, arXiv:1712.00002 [astro-ph.HE]

  52. [60]

    Sensitivity of the Cherenkov Telescope Array to a dark matter signal from the Galactic centre,

    CTA Collaboration, A. Acharyya et al., “Sensitivity of the Cherenkov Telescope Array to a dark matter signal from the Galactic centre,” JCAP 01 (2021) 057, arXiv:2007.16129 [astro-ph.HE]

  53. [61]

    Lepton Number Violation and Massless Nonorthogonal Neutrinos,

    P. Langacker and D. London, “Lepton Number Violation and Massless Nonorthogonal Neutrinos,” Phys. Rev. D 38 (1988) 907

  54. [62]

    General formulae for f (1) → f (2) + γ,

    L. Lavoura, “General formulae for f (1) → f (2) + γ,” Eur. Phys. J. C 29 (2003) 191–195, arXiv:hep-ph/0302221

  55. [63]

    Exact one-loop results for li → ljγ in 3-3-1 models,

    L. T. Hue, L. D. Ninh, T. T. Thuc, and N. T. T. Dat, “Exact one-loop results for li → ljγ in 3-3-1 models,” Eur. Phys. J. C 78 no. 2, (2018) 128, arXiv:1708.09723 [hep-ph]

  56. [64]

    Search for the lepton flavour violating decay µ+ → e+γ with the full dataset of the MEG experiment,

    MEG Collaboration, A. M. Baldini et al., “Search for the lepton flavour violating decay µ+ → e+γ with the full dataset of the MEG experiment,” Eur. Phys. J. C 76 no. 8, (2016) 434, arXiv:1605.05081 [hep-ex]

  57. [65]

    Global constraints on absolute neutrino masses and their ordering,

    F. Capozzi, E. Di Valentino, E. Lisi, A. Marrone, A. Melchiorri, and A. Palazzo, “Global constraints on absolute neutrino masses and their ordering,” Phys. Rev. D 95 no. 9, (2017) 096014, arXiv:2003.08511 [hep-ph] . [Addendum: Phys.Rev.D 101, 116013 (2020)]

  58. [66]

    The fate of hints: updated global analysis of three-flavor neutrino oscillations,

    I. Esteban, M. C. Gonzalez-Garcia, M. Maltoni, T. Schwetz, and A. Zhou, “The fate of hints: updated global analysis of three-flavor neutrino oscillations,” JHEP 09 (2020) 178, arXiv:2007.14792 [hep-ph]

  59. [67]

    Oscillating neutrinos and µ → e, γ,

    J. A. Casas and A. Ibarra, “Oscillating neutrinos and µ → e, γ,” Nucl. Phys. B 618 (2001) 171–204, arXiv:hep-ph/0103065

  60. [68]

    Neutrino phenomenology: The Case of two right-handed neutrinos,

    A. Ibarra and G. G. Ross, “Neutrino phenomenology: The Case of two right-handed neutrinos,” Phys. Lett. B 591 (2004) 285–296, arXiv:hep-ph/0312138

  61. [69]

    Phenomenological consistency of the singlet-triplet scotogenic model,

    D. Restrepo and A. Rivera, “Phenomenological consistency of the singlet-triplet scotogenic model,” JHEP 04 (2020) 134, arXiv:1907.11938 [hep-ph]

  62. [70]

    General parametrization of Majorana neutrino mass models,

    I. Cordero-Carri ´on, M. Hirsch, and A. Vicente, “General parametrization of Majorana neutrino mass models,” Phys. Rev. D 101 no. 7, (2020) 075032, arXiv:1912.08858 [hep-ph]

  63. [71]

    Dirac-Phase Thermal Leptogenesis in the extended Type-I Seesaw Model,

    M. J. Dolan, T. P. Dutka, and R. R. V olkas, “Dirac-Phase Thermal Leptogenesis in the extended Type-I Seesaw Model,” JCAP 06 (2018) 012, arXiv:1802.08373 [hep-ph]

  64. [72]

    Universal inverse seesaw mechanism as a source of the SM fermion mass hierarchy,

    A. E. C. Hern ´andez, D. T. Huong, and I. Schmidt, “Universal inverse seesaw mechanism as a source of the SM fermion mass hierarchy,” Eur. Phys. J. C 82 no. 1, (2022) 63, arXiv:2109.12118 [hep-ph]

  65. [73]

    Determining Horizontal Symmetry from Neutrino Mixing,

    C. S. Lam, “Determining Horizontal Symmetry from Neutrino Mixing,” Phys. Rev. Lett. 101 (2008) 121602, arXiv:0804.2622 [hep-ph]

  66. [74]

    Revisiting Bimaximal Neutrino Mixing in a Model with S(4) Discrete Symmetry,

    G. Altarelli, F. Feruglio, and L. Merlo, “Revisiting Bimaximal Neutrino Mixing in a Model with S(4) Discrete Symmetry,” JHEP 05 (2009) 020, arXiv:0903.1940 [hep-ph]

  67. [75]

    Phenomenological Consequences of See-Saw in S(4) Based Models,

    F. Bazzocchi, L. Merlo, and S. Morisi, “Phenomenological Consequences of See-Saw in S(4) Based Models,” Phys. Rev. D 80 (2009) 053003, arXiv:0902.2849 [hep-ph]

  68. [76]

    Fermion Masses and Mixings in a S(4)-based Model,

    F. Bazzocchi, L. Merlo, and S. Morisi, “Fermion Masses and Mixings in a S(4)-based Model,” Nucl. Phys. B 816 (2009) 204–226, arXiv:0901.2086 [hep-ph]

  69. [77]

    The Interplay Between GUT and Flavour Symmetries in a Pati-Salam x S4 Model,

    R. de Adelhart Toorop, F. Bazzocchi, and L. Merlo, “The Interplay Between GUT and Flavour Symmetries in a Pati-Salam x S4 Model,” JHEP 08 (2010) 001, arXiv:1003.4502 [hep-ph]

  70. [78]

    An SO(10)XS4 Model of Quark-Lepton Complementarity,

    K. M. Patel, “An SO(10)XS4 Model of Quark-Lepton Complementarity,” Phys. Lett. B 695 (2011) 225–230, arXiv:1008.5061 [hep-ph] . 94 CHAPTER 7. BIBLIOGRAPHY

  71. [79]

    Model for T2K indication with maximal atmospheric angle and tri-maximal solar angle,

    S. Morisi, K. M. Patel, and E. Peinado, “Model for T2K indication with maximal atmospheric angle and tri-maximal solar angle,” Phys. Rev. D 84 (2011) 053002, arXiv:1107.0696 [hep-ph]

  72. [80]

    Discrete Flavour Groups, theta13 and Lepton Flavour Violation,

    G. Altarelli, F. Feruglio, L. Merlo, and E. Stamou, “Discrete Flavour Groups, theta13 and Lepton Flavour Violation,”JHEP 08 (2012) 021, arXiv:1205.4670 [hep-ph]

  73. [81]

    S4 Flavored CP Symmetry for Neutrinos,

    R. N. Mohapatra and C. C. Nishi, “ S4 Flavored CP Symmetry for Neutrinos,” Phys. Rev. D 86 (2012) 073007, arXiv:1208.2875 [hep-ph]

  74. [82]

    θ13 and Proton Decay in a Minimal SO(10) × S4 model of Flavor,

    P. S. Bhupal Dev, B. Dutta, R. N. Mohapatra, and M. Severson, “θ13 and Proton Decay in a Minimal SO(10) × S4 model of Flavor,” Phys. Rev. D 86 (2012) 035002, arXiv:1202.4012 [hep-ph]

  75. [83]

    Flavour models for T M1 lepton mixing,

    I. de Medeiros Varzielas and L. Lavoura, “Flavour models for T M1 lepton mixing,” J. Phys. G 40 (2013) 085002, arXiv:1212.3247 [hep-ph]

  76. [84]

    Spontaneous CP violation from vacuum alignment in S4 models of leptons,

    G.-J. Ding, S. F. King, C. Luhn, and A. J. Stuart, “Spontaneous CP violation from vacuum alignment in S4 models of leptons,” JHEP 05 (2013) 084, arXiv:1303.6180 [hep-ph]

  77. [85]

    Neutrino masses and mixing fromS4 flavor twisting,

    H. Ishimori, Y . Shimizu, M. Tanimoto, and A. Watanabe, “Neutrino masses and mixing fromS4 flavor twisting,” Phys. Rev. D 83 (2011) 033004, arXiv:1010.3805 [hep-ph]

  78. [86]

    Dirac Neutrinos with S4 Flavor Symmetry in Warped Extra Dimensions,

    G.-J. Ding and Y .-L. Zhou, “Dirac Neutrinos with S4 Flavor Symmetry in Warped Extra Dimensions,” Nucl. Phys. B 876 (2013) 418–452, arXiv:1304.2645 [hep-ph]

  79. [87]

    Leptons in Holographic Composite Higgs Models with Non-Abelian Discrete Symmetries,

    C. Hagedorn and M. Serone, “Leptons in Holographic Composite Higgs Models with Non-Abelian Discrete Symmetries,” JHEP 10 (2011) 083, arXiv:1106.4021 [hep-ph]

  80. [88]

    Higgs → µτ as an indication for S4 flavor symmetry,

    M. D. Campos, A. E. C ´arcamo Hern´andez, H. P¨as, and E. Schumacher, “Higgs → µτ as an indication for S4 flavor symmetry,” Phys. Rev. D 91 no. 11, (2015) 116011, arXiv:1408.1652 [hep-ph]

  81. [89]

    The 3-3-1 model withS4 flavor symmetry,

    P. V . Dong, H. N. Long, D. V . Soa, and V . V . Vien, “The 3-3-1 model withS4 flavor symmetry,” Eur. Phys. J. C 71 (2011) 1544, arXiv:1009.2328 [hep-ph]

  82. [90]

    Neutrino Mixing with Non-Zeroθ13 and CP Violation in the 3-3-1 Model Based on S4 Flavor Symmetry,

    V . V . Vien, H. N. Long, and D. P. Khoi, “Neutrino Mixing with Non-Zeroθ13 and CP Violation in the 3-3-1 Model Based on S4 Flavor Symmetry,” Int. J. Mod. Phys. A 30 no. 17, (2015) 1550102, arXiv:1506.06063 [hep-ph]

  83. [91]

    SO(10) × S4 grand unified theory of flavour and leptogenesis,

    F. J. de Anda, S. F. King, and E. Perdomo, “SO(10) × S4 grand unified theory of flavour and leptogenesis,” JHEP 12 (2017) 075, arXiv:1710.03229 [hep-ph] . [Erratum: JHEP 04, 069 (2019)]

  84. [92]

    An S4 × SU (5) SUSY GUT of flavour in 6d,

    F. J. de Anda and S. F. King, “An S4 × SU (5) SUSY GUT of flavour in 6d,” JHEP 07 (2018) 057, arXiv:1803.04978 [hep-ph]

  85. [93]

    Littlest Inverse Seesaw Model,

    A. E. C ´arcamo Hern´andez and S. F. King, “Littlest Inverse Seesaw Model,”Nucl. Phys. B 953 (2020) 114950, arXiv:1903.02565 [hep-ph]

  86. [94]

    A New Littlest Seesaw Model,

    P.-T. Chen, G.-J. Ding, S. F. King, and C.-C. Li, “A New Littlest Seesaw Model,”J. Phys. G 47 no. 6, (2020) 065001, arXiv:1906.11414 [hep-ph]

  87. [95]

    Multiple modular symmetries as the origin of flavor,

    I. de Medeiros Varzielas, S. F. King, and Y .-L. Zhou, “Multiple modular symmetries as the origin of flavor,” Phys. Rev. D 101 no. 5, (2020) 055033, arXiv:1906.02208 [hep-ph]

  88. [96]

    Effective alignments and the landscape ofS4 flavour models,

    I. De Medeiros Varzielas, M. Levy, and Y .-L. Zhou, “Effective alignments and the landscape ofS4 flavour models,” Phys. Rev. D 100 no. 3, (2019) 035027, arXiv:1903.10506 [hep-ph]

  89. [97]

    Fermion masses and mixings and some phenomenological aspects of a 3-3-1 model with linear seesaw mechanism,

    A. E. C ´arcamo Hern´andez, N. A. P´erez-Julve, and Y . Hidalgo Vel´asquez, “Fermion masses and mixings and some phenomenological aspects of a 3-3-1 model with linear seesaw mechanism,” Phys. Rev. D 100 no. 9, (2019) 095025, arXiv:1907.13083 [hep-ph]

  90. [98]

    Soft breaking of the µ ↔ τ symmetry by S4 ⊗ Z2,

    J. D. Garc ´ıa-Aguilar, A. E. P. Ram´ırez, M. M. S. Casta˜neda, and J. C. G´omez-Izquierdo, “Soft breaking of the µ ↔ τ symmetry by S4 ⊗ Z2,” arXiv:2209.01316 [hep-ph] . Bibliography 95

  91. [99]

    Symmetry breaking patterns in 3HDM,

    I. P. Ivanov and C. C. Nishi, “Symmetry breaking patterns in 3HDM,” JHEP 01 (2015) 021, arXiv:1410.6139 [hep-ph]

  92. [100]

    First Search for the Majorana Nature of Neutrinos in the Inverted Mass Ordering Region with KamLAND-Zen,

    KamLAND-Zen Collaboration, S. Abe et al., “First Search for the Majorana Nature of Neutrinos in the Inverted Mass Ordering Region with KamLAND-Zen,” arXiv:2203.02139 [hep-ex]

  93. [101]

    The Flavor symmetry,

    J. Kubo, A. Mondragon, M. Mondragon, and E. Rodriguez-Jauregui, “The Flavor symmetry,” Prog. Theor. Phys. 109 (2003) 795–807, arXiv:hep-ph/0302196. [Erratum: Prog.Theor.Phys. 114, 287–287 (2005)]

  94. [102]

    Conditions for vacuum stability in an S(3) extension of the standard model,

    O. F. Beltran, M. Mondragon, and E. Rodriguez-Jauregui, “Conditions for vacuum stability in an S(3) extension of the standard model,” J. Phys. Conf. Ser. 171 (2009) 012028

  95. [103]

    Review of Particle Physics,

    Particle Data Group Collaboration, R. L. Workman and Others, “Review of Particle Physics,”PTEP 2022 (2022) 083C01

  96. [104]

    Resummed Effective Lagrangian for Higgs Mediated FCNC Interactions in the CP Violating MSSM,

    A. Dedes and A. Pilaftsis, “Resummed Effective Lagrangian for Higgs Mediated FCNC Interactions in the CP Violating MSSM,”Phys. Rev. D 67 (2003) 015012, arXiv:hep-ph/0209306

  97. [105]

    Three generations of Higgses and the cyclic groups,

    A. Aranda, C. Bonilla, and J. L. Diaz-Cruz, “Three generations of Higgses and the cyclic groups,” Phys. Lett. B 717 (2012) 248–251, arXiv:1204.5558 [hep-ph]

  98. [106]

    On the ultimate precision of meson mixing observables,

    T. Jubb, M. Kirk, A. Lenz, and G. Tetlalmatzi-Xolocotzi, “On the ultimate precision of meson mixing observables,” Nucl. Phys. B 915 (2017) 431–453, arXiv:1603.07770 [hep-ph]

  99. [107]

    CP violation in the B0 s system,

    M. Artuso, G. Borissov, and A. Lenz, “CP violation in the B0 s system,” Rev. Mod. Phys. 88 no. 4, (2016) 045002, arXiv:1511.09466 [hep-ph] . [Addendum: Rev.Mod.Phys. 91, 049901 (2019)]

  100. [108]

    Averages of b-hadron, c-hadron, and τ-lepton properties as of 2018,

    HFLA VCollaboration, Y . S. Amhiset al., “Averages of b-hadron, c-hadron, and τ-lepton properties as of 2018,” Eur. Phys. J. C 81 no. 3, (2021) 226, arXiv:1909.12524 [hep-ex]

  101. [109]

    Results for the mass difference between the long- and short- lived K mesons for physical quark masses,

    B. Wang, “Results for the mass difference between the long- and short- lived K mesons for physical quark masses,” PoS LATTICE2018 (2019) 286, arXiv:1812.05302 [hep-lat]

  102. [110]

    Measurement of the K(L) - K(S) mass difference using semileptonic decays of tagged neutral kaons,

    CPLEAR Collaboration, A. Angelopoulos et al., “Measurement of the K(L) - K(S) mass difference using semileptonic decays of tagged neutral kaons,” Phys. Lett. B 444 (1998) 38–42

  103. [111]

    Model-independent bounds on new physics effects in non-leptonic tree-level decays of B-mesons,

    A. Lenz and G. Tetlalmatzi-Xolocotzi, “Model-independent bounds on new physics effects in non-leptonic tree-level decays of B-mesons,” JHEP 07 (2020) 177, arXiv:1912.07621 [hep-ph]

  104. [112]

    FLAG Review 2021,

    Flavour Lattice Averaging Group (FLAG)Collaboration, Y . Aokiet al., “FLAG Review 2021,”Eur. Phys. J. C 82 no. 10, (2022) 869, arXiv:2111.09849 [hep-lat]

  105. [113]

    Estimation of oblique electroweak corrections,

    M. E. Peskin and T. Takeuchi, “Estimation of oblique electroweak corrections,” Phys. Rev. D 46 (1992) 381–409

  106. [114]

    Vacuum polarization effects of new physics on electroweak processes,

    G. Altarelli and R. Barbieri, “Vacuum polarization effects of new physics on electroweak processes,” Phys. Lett. B 253 (1991) 161–167

  107. [115]

    Electroweak symmetry breaking after LEP-1 and LEP-2,

    R. Barbieri, A. Pomarol, R. Rattazzi, and A. Strumia, “Electroweak symmetry breaking after LEP-1 and LEP-2,” Nucl. Phys. B 703 (2004) 127–146, arXiv:hep-ph/0405040

  108. [116]

    The Seesaw mechanism at arbitrary order: Disentangling the small scale from the large scale,

    W. Grimus and L. Lavoura, “The Seesaw mechanism at arbitrary order: Disentangling the small scale from the large scale,” JHEP 11 (2000) 042, arXiv:hep-ph/0008179

  109. [117]

    A Precision constraint on multi-Higgs-doublet models,

    W. Grimus, L. Lavoura, O. M. Ogreid, and P. Osland, “A Precision constraint on multi-Higgs-doublet models,” J. Phys. G 35 (2008) 075001, arXiv:0711.4022 [hep-ph]

  110. [118]

    The Oblique parameters in multi-Higgs-doublet models,

    W. Grimus, L. Lavoura, O. M. Ogreid, and P. Osland, “The Oblique parameters in multi-Higgs-doublet models,” Nucl. Phys. B 801 (2008) 81–96, arXiv:0802.4353 [hep-ph] . 96 CHAPTER 7. BIBLIOGRAPHY

  111. [119]

    Precision measurements constraints on the number of Higgs doublets,

    A. E. C ´arcamo Hern´andez, S. Kovalenko, and I. Schmidt, “Precision measurements constraints on the number of Higgs doublets,” Phys. Rev. D 91 (2015) 095014, arXiv:1503.03026 [hep-ph]

  112. [120]

    Electroweak precision fit and new physics in light of the W boson mass,

    C.-T. Lu, L. Wu, Y . Wu, and B. Zhu, “Electroweak precision fit and new physics in light of the W boson mass,” Phys. Rev. D 106 no. 3, (2022) 035034, arXiv:2204.03796 [hep-ph]

  113. [121]

    Scrutinizing a hidden SM-like gauge model with corrections to oblique parameters,

    V . Q. Tran, T. T. Q. Nguyen, and T.-C. Yuan, “Scrutinizing a hidden SM-like gauge model with corrections to oblique parameters,” Eur. Phys. J. C 83 no. 4, (2023) 346, arXiv:2208.10971 [hep-ph]

  114. [122]

    Leading two-loop corrections to the Higgs di-photon decay in the Inert Doublet Model,

    M. Aiko, J. Braathen, and S. Kanemura, “Leading two-loop corrections to the Higgs di-photon decay in the Inert Doublet Model,” arXiv:2307.14976 [hep-ph]

  115. [123]

    On the two-loop BSM corrections to h − →γγ in the aligned THDM,

    G. Degrassi and P. Slavich, “On the two-loop BSM corrections to h − →γγ in the aligned THDM,” Eur. Phys. J. C 83 no. 10, (2023) 941, arXiv:2307.02476 [hep-ph]

  116. [124]

    Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector,

    LHC Higgs Cross Section Working Group Collaboration, D. de Florian et al., “Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector,” arXiv:1610.07922 [hep-ph]

  117. [125]

    Higgs Boson Production and Decay at Hadron Colliders,

    M. Spira, “Higgs Boson Production and Decay at Hadron Colliders,” Prog. Part. Nucl. Phys. 95 (2017) 98–159, arXiv:1612.07651 [hep-ph]

  118. [126]

    Higgs Bosons from Two Gluon Annihilation in Proton Proton Collisions,

    H. M. Georgi, S. L. Glashow, M. E. Machacek, and D. V . Nanopoulos, “Higgs Bosons from Two Gluon Annihilation in Proton Proton Collisions,” Phys. Rev. Lett. 40 (1978) 692

  119. [127]

    Impact of Vacuum Stability Constraints on the Phenomenology of Supersymmetric Models,

    W. G. Hollik, G. Weiglein, and J. Wittbrodt, “Impact of Vacuum Stability Constraints on the Phenomenology of Supersymmetric Models,” JHEP 03 (2019) 109, arXiv:1812.04644 [hep-ph]

  120. [128]

    Vacuum Instabilities in the N2HDM,

    P. M. Ferreira, M. M ¨uhlleitner, R. Santos, G. Weiglein, and J. Wittbrodt, “Vacuum Instabilities in the N2HDM,” JHEP 09 (2019) 006, arXiv:1905.10234 [hep-ph]

  121. [129]

    Minimizing Higgs Potentials via Numerical Polynomial Homotopy Continuation,

    M. Maniatis and D. Mehta, “Minimizing Higgs Potentials via Numerical Polynomial Homotopy Continuation,” Eur. Phys. J. Plus 127 (2012) 91, arXiv:1203.0409 [hep-ph]

  122. [130]

    The Fate of the False Vacuum. 1. Semiclassical Theory,

    S. R. Coleman, “The Fate of the False Vacuum. 1. Semiclassical Theory,” Phys. Rev. D 15 (1977) 2929–2936. [Erratum: Phys.Rev.D 16, 1248 (1977)]

  123. [131]

    The Fate of the False Vacuum. 2. First Quantum Corrections,

    C. G. Callan, Jr. and S. R. Coleman, “The Fate of the False Vacuum. 2. First Quantum Corrections,” Phys. Rev. D 16 (1977) 1762–1768

  124. [132]

    Closed-form expressions of the eigen decomposition of 2 x 2 and 3 x 3 Hermitian matrices,

    C.-A. Deledalle, L. Denis, S. Tabti, and F. Tupin, “Closed-form expressions of the eigen decomposition of 2 x 2 and 3 x 3 Hermitian matrices,” research report, Universit´e de Lyon, 2017. https://hal.archives-ouvertes.fr/hal-01501221

  125. [133]

    SARAH 4 : A tool for (not only SUSY) model builders,

    F. Staub, “SARAH 4 : A tool for (not only SUSY) model builders,” Comput. Phys. Commun. 185 (2014) 1773–1790, arXiv:1309.7223 [hep-ph]

  126. [134]

    From Superpotential to Model Files for FeynArts and CalcHep/CompHep,

    F. Staub, “From Superpotential to Model Files for FeynArts and CalcHep/CompHep,” Comput. Phys. Commun. 181 (2010) 1077–1086, arXiv:0909.2863 [hep-ph]

  127. [135]

    Automatic Calculation of supersymmetric Renormalization Group Equations and Self Energies,

    F. Staub, “Automatic Calculation of supersymmetric Renormalization Group Equations and Self Energies,” Comput. Phys. Commun. 182 (2011) 808–833, arXiv:1002.0840 [hep-ph]

  128. [136]

    SARAH 3.2: Dirac Gauginos, UFO output, and more,

    F. Staub, “SARAH 3.2: Dirac Gauginos, UFO output, and more,” Comput. Phys. Commun. 184 (2013) 1792–1809, arXiv:1207.0906 [hep-ph]

  129. [137]

    Exploring new models in all detail with SARAH,

    F. Staub, “Exploring new models in all detail with SARAH,” Adv. High Energy Phys. 2015 (2015) 840780, arXiv:1503.04200 [hep-ph]

  130. [138]

    SPheno, a program for calculating supersymmetric spectra, SUSY particle decays and SUSY particle production at e+ e- colliders,

    W. Porod, “SPheno, a program for calculating supersymmetric spectra, SUSY particle decays and SUSY particle production at e+ e- colliders,” Comput. Phys. Commun. 153 (2003) 275–315, arXiv:hep-ph/0301101. Bibliography 97

  131. [139]

    SPheno 3.1: Extensions including flavour, CP-phases and models beyond the MSSM,

    W. Porod and F. Staub, “SPheno 3.1: Extensions including flavour, CP-phases and models beyond the MSSM,” Comput. Phys. Commun. 183 (2012) 2458–2469, arXiv:1104.1573 [hep-ph]

  132. [140]

    HiggsBounds-5: Testing Higgs Sectors in the LHC 13 TeV Era,

    P. Bechtle, D. Dercks, S. Heinemeyer, T. Klingl, T. Stefaniak, G. Weiglein, and J. Wittbrodt, “HiggsBounds-5: Testing Higgs Sectors in the LHC 13 TeV Era,”Eur. Phys. J. C 80 no. 12, (2020) 1211, arXiv:2006.06007 [hep-ph]

  133. [141]

    Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using pp collisions at √s = 13 TeV,

    ATLAS Collaboration, G. Aad et al., “Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using pp collisions at √s = 13 TeV,”Phys. Rev. Lett. 125 no. 5, (2020) 051801, arXiv:2002.12223 [hep-ex]

  134. [142]

    SusHi: A program for the calculation of Higgs production in gluon fusion and bottom-quark annihilation in the Standard Model and the MSSM,

    R. V . Harlander, S. Liebler, and H. Mantler, “SusHi: A program for the calculation of Higgs production in gluon fusion and bottom-quark annihilation in the Standard Model and the MSSM,” Comput. Phys. Commun. 184 (2013) 1605–1617, arXiv:1212.3249 [hep-ph]

  135. [143]

    SusHi Bento: Beyond NNLO and the heavy-top limit,

    R. V . Harlander, S. Liebler, and H. Mantler, “SusHi Bento: Beyond NNLO and the heavy-top limit,” Comput. Phys. Commun. 212 (2017) 239–257, arXiv:1605.03190 [hep-ph]

  136. [144]

    Exclusive Signals of an Extended Higgs Sector,

    N. Craig and S. Thomas, “Exclusive Signals of an Extended Higgs Sector,” JHEP 11 (2012) 083, arXiv:1207.4835 [hep-ph]

  137. [145]

    QCD corrections to production of Higgs pseudoscalars,

    R. P. Kauffman and W. Schaffer, “QCD corrections to production of Higgs pseudoscalars,” Phys. Rev. D 49 (1994) 551–554, arXiv:hep-ph/9305279

  138. [146]

    SUSY Higgs production at proton colliders,

    M. Spira, A. Djouadi, D. Graudenz, and P. M. Zerwas, “SUSY Higgs production at proton colliders,” Phys. Lett. B 318 (1993) 347–353

  139. [147]

    Higgs boson production at the LHC,

    M. Spira, A. Djouadi, D. Graudenz, and P. M. Zerwas, “Higgs boson production at the LHC,” Nucl. Phys. B 453 (1995) 17–82, arXiv:hep-ph/9504378

  140. [148]

    Production of a pseudoscalar Higgs boson at hadron colliders at next-to-next-to leading order,

    R. V . Harlander and W. B. Kilgore, “Production of a pseudoscalar Higgs boson at hadron colliders at next-to-next-to leading order,” JHEP 10 (2002) 017, arXiv:hep-ph/0208096

  141. [149]

    Pseudoscalar Higgs boson production at hadron colliders in NNLO QCD,

    C. Anastasiou and K. Melnikov, “Pseudoscalar Higgs boson production at hadron colliders in NNLO QCD,” Phys. Rev. D 67 (2003) 037501, arXiv:hep-ph/0208115

  142. [150]

    HiggsSignals-2: Probing new physics with precision Higgs measurements in the LHC 13 TeV era,

    P. Bechtle, S. Heinemeyer, T. Klingl, T. Stefaniak, G. Weiglein, and J. Wittbrodt, “HiggsSignals-2: Probing new physics with precision Higgs measurements in the LHC 13 TeV era,”Eur. Phys. J. C 81 no. 2, (2021) 145, arXiv:2012.09197 [hep-ph]

  143. [151]

    Applying Exclusion Likelihoods from LHC Searches to Extended Higgs Sectors,

    P. Bechtle, S. Heinemeyer, O. Stal, T. Stefaniak, and G. Weiglein, “Applying Exclusion Likelihoods from LHC Searches to Extended Higgs Sectors,” Eur. Phys. J. C 75 no. 9, (2015) 421, arXiv:1507.06706 [hep-ph]

  144. [152]

    Review of particle physics,

    Particle Data Group Collaboration, S. Navas et al., “Review of particle physics,”Phys. Rev. D 110 no. 3, (2024) 030001

  145. [153]

    Comparison of statistical sampling methods with ScannerBit, the GAMBIT scanning module,

    GAMBIT Collaboration, G. D. Martinez, J. McKay, B. Farmer, P. Scott, E. Roebber, A. Putze, and J. Conrad, “Comparison of statistical sampling methods with ScannerBit, the GAMBIT scanning module,” Eur. Phys. J. C 77 no. 11, (2017) 761, arXiv:1705.07959 [hep-ph]

  146. [154]

    Pippi - painless parsing, post-processing and plotting of posterior and likelihood samples,

    P. Scott, “Pippi - painless parsing, post-processing and plotting of posterior and likelihood samples,” Eur. Phys. J. Plus 127 (2012) 138, arXiv:1206.2245 [physics.data-an]

  147. [155]

    Radiative seesaw mechanism at weak scale,

    Z.-j. Tao, “Radiative seesaw mechanism at weak scale,” Phys. Rev. D 54 (1996) 5693–5697, arXiv:hep-ph/9603309

  148. [156]

    Indirect detection constraints on the scotogenic dark matter model,

    T. de Boer, R. Busse, A. Kappes, M. Klasen, and S. Zeinstra, “Indirect detection constraints on the scotogenic dark matter model,” JCAP 08 (2021) 038, arXiv:2105.04899 [hep-ph] . 98 CHAPTER 7. BIBLIOGRAPHY

  149. [157]

    Dark Matter through the Higgs portal,

    G. Arcadi, A. Djouadi, and M. Raidal, “Dark Matter through the Higgs portal,” Phys. Rept. 842 (2020) 1–180, arXiv:1903.03616 [hep-ph]

  150. [158]

    Particle dark matter: Evidence, candidates and constraints,

    G. Bertone, D. Hooper, and J. Silk, “Particle dark matter: Evidence, candidates and constraints,” Phys. Rept. 405 (2005) 279–390, arXiv:hep-ph/0404175

  151. [159]

    micrOMEGAs 3: A program for calculating dark matter observables,

    G. Belanger, F. Boudjema, A. Pukhov, and A. Semenov, “micrOMEGAs 3: A program for calculating dark matter observables,” Comput. Phys. Commun. 185 (2014) 960–985, arXiv:1305.0237 [hep-ph]

  152. [160]

    micrOMEGAs4.1: two dark matter candidates,

    G. B ´elanger, F. Boudjema, A. Pukhov, and A. Semenov, “micrOMEGAs4.1: two dark matter candidates,” Comput. Phys. Commun. 192 (2015) 322–329, arXiv:1407.6129 [hep-ph]

  153. [161]

    Collider limits on new physics within micrOMEGAs 4.3,

    D. Barducci, G. Belanger, J. Bernon, F. Boudjema, J. Da Silva, S. Kraml, U. Laa, and A. Pukhov, “Collider limits on new physics within micrOMEGAs 4.3,” Comput. Phys. Commun. 222 (2018) 327–338, arXiv:1606.03834 [hep-ph]

  154. [162]

    micrOMEGAs5.0 : Freeze-in,

    G. B ´elanger, F. Boudjema, A. Goudelis, A. Pukhov, and B. Zaldivar, “micrOMEGAs5.0 : Freeze-in,” Comput. Phys. Commun. 231 (2018) 173–186, arXiv:1801.03509 [hep-ph]

  155. [163]

    DarkBit: A GAMBIT module for computing dark matter observables and likelihoods,

    GAMBIT Dark Matter Workgroup Collaboration, T. Bringmann et al., “DarkBit: A GAMBIT module for computing dark matter observables and likelihoods,” Eur. Phys. J. C 77 no. 12, (2017) 831, arXiv:1705.07920 [hep-ph]

  156. [164]

    Global analyses of Higgs portal singlet dark matter models using GAMBIT,

    GAMBIT Collaboration, P. Athron et al., “Global analyses of Higgs portal singlet dark matter models using GAMBIT,” Eur. Phys. J. C 79 no. 1, (2019) 38, arXiv:1808.10465 [hep-ph]

  157. [165]

    First Dark Matter Search with Nuclear Recoils from the XENONnT Experiment,

    XENON Collaboration, E. Aprile et al., “First Dark Matter Search with Nuclear Recoils from the XENONnT Experiment,” Phys. Rev. Lett. 131 no. 4, (2023) 041003, arXiv:2303.14729 [hep-ex]

  158. [166]

    Dark matter sensitivity of multi-ton liquid xenon detectors,

    M. Schumann, L. Baudis, L. B ¨utikofer, A. Kish, and M. Selvi, “Dark matter sensitivity of multi-ton liquid xenon detectors,” JCAP 10 (2015) 016, arXiv:1506.08309 [physics.ins-det]

  159. [167]

    Implication of neutrino backgrounds on the reach of next generation dark matter direct detection experiments,

    J. Billard, L. Strigari, and E. Figueroa-Feliciano, “Implication of neutrino backgrounds on the reach of next generation dark matter direct detection experiments,” Phys. Rev. D 89 no. 2, (2014) 023524, arXiv:1307.5458 [hep-ph]

  160. [168]

    Inert Doublet Model in light of LHC Run I and astrophysical data,

    A. Ilnicka, M. Krawczyk, and T. Robens, “Inert Doublet Model in light of LHC Run I and astrophysical data,” Phys. Rev. D 93 no. 5, (2016) 055026, arXiv:1508.01671 [hep-ph]

  161. [169]

    Testing the dark matter scenario in the inert doublet model by future precision measurements of the Higgs boson couplings,

    S. Kanemura, M. Kikuchi, and K. Sakurai, “Testing the dark matter scenario in the inert doublet model by future precision measurements of the Higgs boson couplings,” Phys. Rev. D 94 no. 11, (2016) 115011, arXiv:1605.08520 [hep-ph]

  162. [170]

    Dark matter in a singlet-extended inert Higgs-doublet model,

    M. O. Khojali, A. Abdalgabar, A. Ahriche, and A. S. Cornell, “Dark matter in a singlet-extended inert Higgs-doublet model,” Phys. Rev. D 106 no. 9, (2022) 095039, arXiv:2206.06211 [hep-ph]

  163. [171]

    Neutrino Mass and Baryon Number Nonconservation in Superstring Models,

    R. Mohapatra and J. W. F. Valle, “Neutrino Mass and Baryon Number Nonconservation in Superstring Models,” Phys.Rev.D 34 (1986) 1642

  164. [172]

    Hierarchy of Quark Masses, Cabibbo Angles and CP Violation,

    C. D. Froggatt and H. B. Nielsen, “Hierarchy of Quark Masses, Cabibbo Angles and CP Violation,” Nucl. Phys. B 147 (1979) 277–298

  165. [173]

    Predictive extended 3HDM with S4 family symmetry,

    A. E. C ´arcamo Hern´andez, C. Espinoza, J. C. G´omez-Izquierdo, J. M. Gonz´alez, and M. Mondrag´on, “Predictive extended 3HDM with S4 family symmetry,” arXiv:2212.12000 [hep-ph]

  166. [174]

    Interesting radiative patterns of neutrino mass in an SU(3)(C) x SU(3)(L) x U(1)(X) model with right-handed neutrinos,

    D. Chang and H. N. Long, “Interesting radiative patterns of neutrino mass in an SU(3)(C) x SU(3)(L) x U(1)(X) model with right-handed neutrinos,” Phys. Rev. D73 (2006) 053006, arXiv:hep-ph/0603098 [hep-ph]. Bibliography 99

  167. [175]

    A variant of 3-3-1 model for the generation of the SM fermion mass and mixing pattern,

    A. E. C ´arcamo Hern´andez, S. Kovalenko, H. N. Long, and I. Schmidt, “A variant of 3-3-1 model for the generation of the SM fermion mass and mixing pattern,” JHEP 07 (2018) 144, arXiv:1705.09169 [hep-ph]

  168. [176]

    Minimal model for the fermion flavor structure, mass hierarchy, dark matter, leptogenesis, and the electron and muon anomalous magnetic moments,

    A. E. C ´arcamo Hern´andez, D. T. Huong, and H. N. Long, “Minimal model for the fermion flavor structure, mass hierarchy, dark matter, leptogenesis, and the electron and muon anomalous magnetic moments,”Phys. Rev. D 102 no. 5, (2020) 055002, arXiv:1910.12877 [hep-ph]

  169. [177]

    Non-Abelian Discrete Symmetries in Particle Physics,

    H. Ishimori, T. Kobayashi, H. Ohki, Y . Shimizu, H. Okada, and M. Tanimoto, “Non-Abelian Discrete Symmetries in Particle Physics,” Prog. Theor. Phys. Suppl. 183 (2010) 1–163, arXiv:1003.3552 [hep-th]

  170. [178]

    Lepton Number Violation With Quasi Dirac Neutrinos,

    J. W. F. Valle and M. Singer, “Lepton Number Violation With Quasi Dirac Neutrinos,”Phys. Rev. D28 (1983) 540

  171. [179]

    The 331 model with right handed neutrinos,

    H. N. Long, “The 331 model with right handed neutrinos,” Phys. Rev. D 53 (1996) 437–445, arXiv:hep-ph/9504274

  172. [180]

    Novel supersymmetric SO(10) seesaw mechanism,

    M. Malinsky, J. C. Romao, and J. W. F. Valle, “Novel supersymmetric SO(10) seesaw mechanism,”Phys. Rev. Lett. 95 (2005) 161801, arXiv:hep-ph/0506296

  173. [181]

    Enhancement of H → γγ in SU (5) model with 45H 1 plet,

    S. Khalil and S. Salem, “Enhancement of H → γγ in SU (5) model with 45H 1 plet,” Nucl. Phys. B 876 (2013) 473–492, arXiv:1304.3689 [hep-ph]

  174. [182]

    Constraining Flavor Changing Interactions from LHC Run-2 Dilepton Bounds with Vector Mediators,

    F. S. Queiroz, C. Siqueira, and J. W. F. Valle, “Constraining Flavor Changing Interactions from LHC Run-2 Dilepton Bounds with Vector Mediators,”Phys. Lett. B 763 (2016) 269–274, arXiv:1608.07295 [hep-ph]

  175. [183]

    331 Models Facing the Tensions in ∆F = 2 Processes with the Impact on ε′/ε, Bs → µ+µ− and B → K ∗µ+µ−,

    A. J. Buras and F. De Fazio, “331 Models Facing the Tensions in ∆F = 2 Processes with the Impact on ε′/ε, Bs → µ+µ− and B → K ∗µ+µ−,” JHEP 08 (2016) 115, arXiv:1604.02344 [hep-ph]

  176. [184]

    CP4 miracle: shaping Yukawa sector with CP symmetry of order four,

    P. M. Ferreira, I. P. Ivanov, E. Jim´enez, R. Pasechnik, and H. Serˆodio, “CP4 miracle: shaping Yukawa sector with CP symmetry of order four,” JHEP 01 (2018) 065, arXiv:1711.02042 [hep-ph]

  177. [185]

    Nondecoupling of charged scalars in Higgs decay to two photons and symmetries of the scalar potential,

    G. Bhattacharyya and D. Das, “Nondecoupling of charged scalars in Higgs decay to two photons and symmetries of the scalar potential,” Phys. Rev. D 91 (2015) 015005, arXiv:1408.6133 [hep-ph]

  178. [186]

    TASI 2013 lectures on Higgs physics within and beyond the Standard Model,

    H. E. Logan, “TASI 2013 lectures on Higgs physics within and beyond the Standard Model,” arXiv:1406.1786 [hep-ph]

  179. [187]

    A renormalizable left-right symmetric model with low scale seesaw mechanisms,

    A. E. C. Hern ´andez and I. Schmidt, “A renormalizable left-right symmetric model with low scale seesaw mechanisms,” arXiv:2101.02718 [hep-ph]

  180. [188]

    Recent measurements of higgs boson properties in the diphoton decay channel with the cms detector,

    P. Saha, “Recent measurements of higgs boson properties in the diphoton decay channel with the cms detector,” in Proceedings of the XXIV DAE-BRNS High Energy Physics Symposium, Jatni, India, B. Mohanty, S. K. Swain, R. Singh, and V . K. S. Kashyap, eds., pp. 183–186. Springer ...

  181. [189]

    Measurement of the properties of Higgs boson production at √s = 13 TeV in the H → γγ channel using 139 fb−1 of pp collision data with the ATLAS experiment,

    ATLAS Collaboration, “Measurement of the properties of Higgs boson production at √s = 13 TeV in the H → γγ channel using 139 fb−1 of pp collision data with the ATLAS experiment,” arXiv:2207.00348 [hep-ex]

  182. [190]

    S, T, U parameters in SU(3)(C) x SU(3)(L) x U(1) model with right-handed neutrinos,

    H. N. Long and T. Inami, “S, T, U parameters in SU(3)(C) x SU(3)(L) x U(1) model with right-handed neutrinos,” Phys. Rev. D 61 (2000) 075002, arXiv:hep-ph/9902475

  183. [191]

    Some phenomenological aspects of the 3-3-1 model with the C´arcamo-Kovalenko-Schmidt mechanism,

    H. N. Long, N. V . Hop, L. T. Hue, N. H. Thao, and A. E. C´arcamo Hern´andez, “Some phenomenological aspects of the 3-3-1 model with the C´arcamo-Kovalenko-Schmidt mechanism,”Phys. Rev. D 100 no. 1, (2019) 015004, arXiv:1810.00605 [hep-ph]

  184. [192]

    W-mass anomaly in the simplest linear seesaw mechanism,

    A. Batra, P. Bharadwaj, S. Mandal, R. Srivastava, and J. W. F. Valle, “W-mass anomaly in the simplest linear seesaw mechanism,” Phys. Lett. B 834 (2022) 137408, arXiv:2208.04983 [hep-ph] . Appendix A Symmetry groups A.1 Discrete symmetry groups. Imagine having an object with a...

Pith tools