[1] P. A. Zyla et al. [Particle Data Group], “Review of Particle Physics,” PTEP 2020, no.8, 083C01 (2020).
[2] B. D. Fields, K. A. Olive, T. H. Yeh and C. Young, JCAP 03, 010 (2020) [erratum: JCAP 11, E02 (2020)] [arXiv:1912.01132 [astro-ph.CO]].
[3] N. Aghanim et al. [Planck], “Planck 2018 results. VI. Cosmological parameters,” Astron. Astrophys. 641, A6 (2020) [erratum: Astron. Astrophys. 652, C4 (2021)] [arXiv:1807.06209 [astro-ph.CO]].
[4] Y. Fukuda et al. [Super-Kamiokande], “Evidence for oscillation of atmospheric neu- trinos,” Phys. Rev. Lett. 81, 1562-1567 (1998) [arXiv:hep-ex/9807003 [hep-ex]].
[5] Q. R. Ahmad et al. [SNO], “Measurement of the rate of νe + d p + p + e− interactions produced by 8B solar neutrinos at the Sudbury Neutrino Observatory,” Phys. Rev. Lett. 87, 071301 (2001) [arXiv:nucl-ex/0106015 [nucl-ex]].
[6] Q. R. Ahmad et al. [SNO], “Direct evidence for neutrino flavor transformation from neutral current interactions in the Sudbury Neutrino Observatory,” Phys. Rev. Lett. 89, 011301 (2002) [arXiv:nucl-ex/0204008 [nucl-ex]].
[7] K. Abe et al. [T2K], “Improved constraints on neutrino mixing from the T2K ex- periment with 3.13 1021 protons on target,” Phys. Rev. D 103, no.11, 112008(2021) [arXiv:2101.03779 [hep-ex]].
[8] M. A. Acero et al. [NOvA], “An Improved Measurement of Neutrino Oscillation Parameters by the NOvA Experiment,” [arXiv:2108.08219 [hep-ex]].
[9] D. Adey et al. [Daya Bay], “Measurement of the Electron Antineutrino Oscillation with 1958 Days of Operation at Daya Bay,” Phys. Rev. Lett. 121, no.24, 241805 (2018) [arXiv:1809.02261 [hep-ex]].
[10] B. Aharmim et al. [SNO], Phys. Rev. C 88, 025501 (2013) doi:10.1103/PhysRevC.88.025501 [arXiv:1109.0763 [nucl-ex]].
[11] S. Weinberg, “A Model of Leptons,” Phys. Rev. Lett. 19, 1264-1266 (1967)
[12] A. Salam, “Weak and Electromagnetic Interactions,” Conf. Proc. C 680519, 367- 377 (1968)
[13] G. Aad et al. [ATLAS], “Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC,” Phys. Lett. B 716, 1-29 (2012) [arXiv:1207.7214 [hep-ex]].
[14] S. Chatrchyan et al. [CMS], “Observation of a New Boson at a Mass of 125 GeV with the CMS Experiment at the LHC,” Phys. Lett. B 716, 30-61 (2012) [arXiv:1207.7235 [hep-ex]].
[15] A. H. Guth, “The Inflationary Universe: A Possible Solution to the Horizon and Flatness Problems,” Phys. Rev. D 23, 347-356 (1981)
[16] K. Sato, “First Order Phase Transition of a Vacuum and Expansion of the Universe,” Mon. Not. Roy. Astron. Soc. 195, 467-479 (1981) NORDITA-80-29.
[17] A. D. Sakharov, “Violation of CP Invariance, C asymmetry, and baryon asymmetry of the universe,” Pisma Zh. Eksp. Teor. Fiz. 5, 32-35 (1967)
[18] M. Yoshimura, “Unified Gauge Theories and the Baryon Number of the Universe,” Phys. Rev. Lett. 41, 281-284 (1978) [erratum: Phys. Rev. Lett. 42, 746 (1979)]
[19] S. Weinberg, “Cosmological Production of Baryons,” Phys. Rev. Lett. 42, 850-853 (1979)
[20] I. Affleck and M. Dine, “A New Mechanism for Baryogenesis,” Nucl. Phys. B 249, 361-380 (1985)
[21] V. A. Kuzmin, V. A. Rubakov and M. E. Shaposhnikov, “On the Anomalous Elec- troweak Baryon Number Nonconservation in the Early Universe,” Phys. Lett. B 155, 36 (1985)
[22] M. Fukugita and T. Yanagida, “Baryogenesis Without Grand Unification,” Phys. Lett. B 174, 45-47 (1986)
[23] F. R. Klinkhamer and N. S. Manton, “A Saddle Point Solution in the Weinberg- Salam Theory,” Phys. Rev. D 30, 2212 (1984)
[24] M. B. Gavela, P. Hernandez, J. Orloff and O. Pene, “Standard model CP viola- tion and baryon asymmetry,” Mod. Phys. Lett. A 9, 795-810 (1994) [arXiv:hep- ph/9312215 [hep-ph]]; M. B. Gavela, M. Lozano, J. Orloff and O. Pene, Nucl. Phys. B 430, 345-381 (1994) [arXiv:hep-ph/9406288 [hep-ph]]; M. B. Gavela, P. Hernan- dez, J. Orloff, O. Pene and C. Quimbay, “Standard model CP violation and baryon asymmetry. Part 2: Finite temperature,” ibid 430, 382-426 (1994) [arXiv:hep- ph/9406289 [hep-ph]].
[25] P. Huet and E. Sather, “Electroweak baryogenesis and standard model CP viola- tion,” Phys. Rev. D 51, 379-394 (1995) [arXiv:hep-ph/9404302 [hep-ph]].
[26] M. E. Shaposhnikov, “Baryon Asymmetry of the Universe in Standard Electroweak Theory,” Nucl. Phys. B 287, 757-775 (1987)
[27] A. I. Bochkarev and M. E. Shaposhnikov, “Electroweak Production of Baryon Asym- metry and Upper Bounds on the Higgs and Top Masses,” Mod. Phys. Lett. A 2, 417 (1987)
[28] K. Kajantie, M. Laine, K. Rummukainen and M. E. Shaposhnikov, “Is there a hot electroweak phase transition at mH ≳ mW ?,” Phys. Rev. Lett. 77, 2887-2890 (1996) [arXiv:hep-ph/9605288 [hep-ph]];
[29] M. D’Onofrio and K. Rummukainen, “Standard model cross-over on the lattice,” Phys. Rev. D 93, no.2, 025003 (2016) [arXiv:1508.07161 [hep-ph]].
[30] G. W. Anderson and L. J. Hall, “The Electroweak phase transition and baryogene- sis,” Phys. Rev. D 45, 2685-2698 (1992)
[31] J. R. Espinosa and M. Quiros, “The Electroweak phase transition with a singlet,” Phys. Lett. B 305, 98-105 (1993) [arXiv:hep-ph/9301285 [hep-ph]].
[32] J. Choi and R. R. Volkas, “Real Higgs singlet and the electroweak phase transition in the Standard Model,” Phys. Lett. B 317, 385-391 (1993) [arXiv:hep-ph/9308234 [hep-ph]].
[33] S. W. Ham, Y. S. Jeong and S. K. Oh, “Electroweak phase transition in an extension of the standard model with a real Higgs singlet,” J. Phys. G 31, no.8, 857-871 (2005) [arXiv:hep-ph/0411352 [hep-ph]].
[34] S. J. Huber, T. Konstandin, T. Prokopec and M. G. Schmidt, “Electroweak Phase Transition and Baryogenesis in the nMSSM,” Nucl. Phys. B 757, 172-196 (2006) [arXiv:hep-ph/0606298 [hep-ph]].
[35] A. Ahriche, “What is the criterion for a strong first order electroweak phase tran- sition in singlet models?,” Phys. Rev. D 75, 083522 (2007) [arXiv:hep-ph/0701192 [hep-ph]].
[36] J. M. Cline, G. Laporte, H. Yamashita and S. Kraml, “Electroweak Phase Tran- sition and LHC Signatures in the Singlet Majoron Model,” JHEP 07, 040 (2009) [arXiv:0905.2559 [hep-ph]].
[37] J. R. Espinosa, T. Konstandin and F. Riva, “Strong Electroweak Phase Transi- tions in the Standard Model with a Singlet,” Nucl. Phys. B 854, 592-630 (2012) [arXiv:1107.5441 [hep-ph]].
[38] J. R. Espinosa, B. Gripaios, T. Konstandin and F. Riva, “Electroweak Baryogenesis in Non-minimal Composite Higgs Models,” JCAP 01, 012 (2012) [arXiv:1110.2876 [hep-ph]].
[39] J. McDonald, “Electroweak baryogenesis and dark matter via a gauge singlet scalar,” Phys. Lett. B 323, 339-346 (1994)
[40] S. Profumo, M. J. Ramsey-Musolf and G. Shaughnessy, “Singlet Higgs phenomenol- ogy and the electroweak phase transition,” JHEP 08, 010 (2007) [arXiv:0705.2425 [hep-ph]].
[41] V. Barger, P. Langacker, M. McCaskey, M. Ramsey-Musolf and G. Shaughnessy, “Complex Singlet Extension of the Standard Model,” Phys. Rev. D 79, 015018 (2009) [arXiv:0811.0393 [hep-ph]].
[42] J. M. Cline and K. Kainulainen, “Electroweak baryogenesis and dark matter from a singlet Higgs,” JCAP 01, 012 (2013) [arXiv:1210.4196 [hep-ph]].
[43] N. Turok and J. Zadrozny, “Electroweak baryogenesis in the two doublet model,” Nucl. Phys. B 358, 471-493 (1991)
[44] J. M. Cline, K. Kainulainen and A. P. Vischer, “Dynamics of two Higgs doublet CP violation and baryogenesis at the electroweak phase transition,” Phys. Rev. D 54, 2451-2472 (1996) [arXiv:hep-ph/9506284 [hep-ph]].
[45] L. Fromme, S. J. Huber and M. Seniuch, “Baryogenesis in the two-Higgs doublet model,” JHEP 11, 038 (2006) [arXiv:hep-ph/0605242 [hep-ph]].
[46] J. M. Cline, K. Kainulainen and M. Trott, “Electroweak Baryogenesis in Two Higgs Doublet Models and B meson anomalies,” JHEP 11, 089 (2011) [arXiv:1107.3559 [hep-ph]].
[47] S. Tulin and P. Winslow, Phys. Rev. D 84, 034013 (2011) doi:10.1103/PhysRevD.84.034013 [arXiv:1105.2848 [hep-ph]].
[48] T. Liu, M. J. Ramsey-Musolf and J. Shu, “Electroweak Beautygenesis: From b to s CP-violation to the Cosmic Baryon Asymmetry,” Phys. Rev. Lett. 108, 221301 (2012) [arXiv:1109.4145 [hep-ph]].
[49] M. Ahmadvand, “Baryogenesis within the two-Higgs-doublet model in the Elec- troweak scale,” Int. J. Mod. Phys. A 29, no.20, 1450090 (2014) [arXiv:1308.3767 [hep-ph]].
[50] C. W. Chiang, K. Fuyuto and E. Senaha, “Electroweak Baryogenesis with Lepton Flavor Violation,” Phys. Lett. B 762, 315-320 (2016) [arXiv:1607.07316 [hep-ph]].
[51] H. K. Guo, Y. Y. Li, T. Liu, M. Ramsey-Musolf and J. Shu, “Lepton-Flavored Elec- troweak Baryogenesis,” Phys. Rev. D 96, no.11, 115034 (2017) [arXiv:1609.09849 [hep-ph]].
[52] K. Fuyuto, W. S. Hou and E. Senaha, “Electroweak baryogenesis driven by extra top Yukawa couplings,” Phys. Lett. B 776, 402-406 (2018) [arXiv:1705.05034 [hep-ph]]; “Cancellation mechanism for the electron electric dipole moment connected with the baryon asymmetry of the Universe,” Phys. Rev. D 101, no.1, 011901 (2020) [arXiv:1910.12404 [hep-ph]].
[53] T. Modak and E. Senaha, “Electroweak baryogenesis via bottom transport,” Phys. Rev. D 99, no.11, 115022 (2019) [arXiv:1811.08088 [hep-ph]]; “Probing Electroweak Baryogenesis induced by extra bottom Yukawa coupling via EDMs and collider sig- natures,” JHEP 11, 025 (2020) [arXiv:2005.09928 [hep-ph]]; “Electroweak baryo- genesis via bottom transport: Complementarity between LHC and future lepton collider probes,” Phys. Lett. B 822, 136695 (2021) [arXiv:2107.12789 [hep-ph]].
[54] P. Basler, M. Mu¨hlleitner and J. Mu¨ller, “Electroweak Baryogenesis in the CP- Violating Two-Higgs Doublet Model,” [arXiv:2108.03580 [hep-ph]].
[55] K. Enomoto, S. Kanemura and Y. Mura, “Electroweak baryogenesis in aligned two Higgs doublet models,” JHEP 01, 104 (2022) [arXiv:2111.13079 [hep-ph]].
[56] T. A. Chowdhury, M. Nemevsek, G. Senjanovic and Y. Zhang, “Dark Matter as the Trigger of Strong Electroweak Phase Transition,” JCAP 02, 029 (2012) [arXiv:1110.5334 [hep-ph]].
[57] D. Borah and J. M. Cline, “Inert Doublet Dark Matter with Strong Electroweak Phase Transition,” Phys. Rev. D 86, 055001 (2012) [arXiv:1204.4722 [hep-ph]].
[58] G. Gil, P. Chankowski and M. Krawczyk, “Inert Dark Matter and Strong Elec- troweak Phase Transition,” Phys. Lett. B 717, 396-402 (2012) [arXiv:1207.0084 [hep-ph]].
[59] H. H. Patel and M. J. Ramsey-Musolf, “Stepping Into Electroweak Symmetry Break- ing: Phase Transitions and Higgs Phenomenology,” Phys. Rev. D 88, 035013 (2013) [arXiv:1212.5652 [hep-ph]].
[60] C. W. Chiang and T. Yamada, “Electroweak phase transition in Georgi–Machacek model,” Phys. Lett. B 735, 295-300 (2014) [arXiv:1404.5182 [hep-ph]].
[61] P. Minkowski, “µ eγ at a Rate of One Out of 109 Muon Decays?,” Phys. Lett. B 67, 421-428 (1977); T. Yanagida, “Horizontal gauge symmetry and masses of neu- trinos,” Conf. Proc. C 7902131, 95-99 (1979); “Horizontal Symmetry and Masses of Neutrinos,” Prog. Theor. Phys. 64, 1103 (1980); M. Gell-Mann, P. Ramond andR. Slansky, “Complex Spinors and Unified Theories,” Conf. Proc. C 790927, 315- 321 (1979) [arXiv:1306.4669 [hep-th]];
[62] R. N. Mohapatra and G. Senjanovic, “Neutrino Mass and Spontaneous Parity Non- conservation,” Phys. Rev. Lett. 44, 912 (1980). J. Schechter and J. W. F. Valle, “Neutrino Masses in SU(2) x U(1) Theories,” Phys. Rev. D 22, 2227 (1980)
[63] W. Konetschny and W. Kummer, “Nonconservation of Total Lepton Number with Scalar Bosons,” Phys. Lett. B 70, 433-435 (1977); M. Magg and C. Wetterich, Phys. Lett. B 94, 61-64 (1980); G. Lazarides, Q. Shafi and C. Wetterich, Nucl. Phys. B 181, 287-300 (1981).
[64] R. Foot, H. Lew, X. G. He and G. C. Joshi, “Seesaw Neutrino Masses Induced by a Triplet of Leptons,” Z. Phys. C 44, 441 (1989)
[65] A. G. Akeroyd and M. Aoki, “Single and pair production of doubly charged Higgs bosons at hadron colliders,” Phys. Rev. D 72, 035011 (2005) [arXiv:hep-ph/0506176 [hep-ph]].
[66] A. G. Akeroyd, M. Aoki and H. Sugiyama, “Lepton Flavour Violating Decays tau anti-l ll and mu e gamma in the Higgs Triplet Model,” Phys. Rev. D 79,113010 (2009) [arXiv:0904.3640 [hep-ph]].
[67] A. G. Akeroyd and H. Sugiyama, “Production of doubly charged scalars from the decay of singly charged scalars in the Higgs Triplet Model,” Phys. Rev. D 84, 035010 (2011) [arXiv:1105.2209 [hep-ph]].
[68] M. Aoki, S. Kanemura and K. Yagyu, “Testing the Higgs triplet model with the mass difference at the LHC,” Phys. Rev. D 85, 055007 (2012) [arXiv:1110.4625 [hep-ph]].
[69] A. Zee, “A Theory of Lepton Number Violation, Neutrino Majorana Mass, and Oscillation,” Phys. Lett. B 93, 389 (1980) [erratum: Phys. Lett. B 95, 461 (1980)]
[70] T. P. Cheng and L. F. Li, “Neutrino Masses, Mixings and Oscillations in SU(2) x U(1) Models of Electroweak Interactions,” Phys. Rev. D 22, 2860 (1980)
[71] A. Zee, “Quantum Numbers of Majorana Neutrino Masses,” Nucl. Phys. B 264, 99-110 (1986)
[72] K. S. Babu, “Model of ’Calculable’ Majorana Neutrino Masses,” Phys. Lett. B 203, 132-136 (1988)
[73] E. Ma, “Verifiable radiative seesaw mechanism of neutrino mass and dark matter,” Phys. Rev. D 73, 077301 (2006) [arXiv:hep-ph/0601225 [hep-ph]].
[74] L. M. Krauss, S. Nasri and M. Trodden, “A Model for neutrino masses and dark matter,” Phys. Rev. D 67, 085002 (2003) [arXiv:hep-ph/0210389 [hep-ph]].
[75] M. Aoki, S. Kanemura and O. Seto, “Neutrino mass, Dark Matter and Baryon Asymmetry via TeV-Scale Physics without Fine-Tuning,” Phys. Rev. Lett. 102, 051805 (2009) [arXiv:0807.0361 [hep-ph]]; “A Model of TeV Scale Physics for Neu- trino Mass, Dark Matter and Baryon Asymmetry and its Phenomenology,” Phys. Rev. D 80, 033007 (2009) [arXiv:0904.3829 [hep-ph]].
[76] M. Gustafsson, J. M. No and M. A. Rivera, “Predictive Model for Radiatively In- duced Neutrino Masses and Mixings with Dark Matter,” Phys. Rev. Lett. 110, no.21, 211802 (2013) [erratum: Phys. Rev. Lett. 112, no.25, 259902 (2014)][arXiv:1212.4806 [hep-ph]]; “Radiative neutrino mass generation linked to neu- trino mixing and 0νββ-decay predictions,” Phys. Rev. D 90, no.1, 013012 (2014) [arXiv:1402.0515 [hep-ph]];
[77] S. M. Davidson and H. E. Logan, “Dirac neutrinos from a second Higgs doublet,” Phys. Rev. D 80, 095008 (2009) [arXiv:0906.3335 [hep-ph]].
[78] S. Nasri and S. Moussa, “Model for small neutrino masses at the TeV scale,” Mod. Phys. Lett. A 17, 771-778 (2002) [arXiv:hep-ph/0106107 [hep-ph]]; S. Kanemura,T. Nabeshima and H. Sugiyama, Phys. Lett. B 703, 66-70 (2011) [arXiv:1106.2480 [hep-ph]].
[79] P. H. Gu and U. Sarkar, “Radiative Neutrino Mass, Dark Matter and Leptogenesis,” Phys. Rev. D 77, 105031 (2008) [arXiv:0712.2933 [hep-ph]].
[80] S. Kanemura, K. Sakurai and H. Sugiyama, “Probing Models of Dirac Neutrino Masses via the Flavor Structure of the Mass Matrix,” Phys. Lett. B 758, 465-472 (2016) [arXiv:1603.08679 [hep-ph]].
[81] S. Kanemura, K. Sakurai and H. Sugiyama, “Neutrino mass without lepton number violation, dark matter; and a strongly first-order phase transition,” Phys. Rev. D 96, no.9, 095024 (2017) [arXiv:1705.07040 [hep-ph]].
[82] K. Enomoto, S. Kanemura, K. Sakurai and H. Sugiyama, “New model for radiatively generated Dirac neutrino masses and lepton flavor violating decays of the Higgs boson,” Phys. Rev. D 100, no.1, 015044 (2019) [arXiv:1904.07039 [hep-ph]].
[83] V. Silveira and A. Zee, “SCALAR PHANTOMS,” Phys. Lett. B 161, 136-140 (1985)
[84] J. McDonald, “Gauge singlet scalars as cold dark matter,” Phys. Rev. D 50, 3637- 3649 (1994) [arXiv:hep-ph/0702143 [hep-ph]].
[85] C. P. Burgess, M. Pospelov and T. ter Veldhuis, “The Minimal model of nonbaryonic dark matter: A Singlet scalar,” Nucl. Phys. B 619, 709-728 (2001) [arXiv:hep- ph/0011335 [hep-ph]].
[86] R. N. Lerner and J. McDonald, “Gauge singlet scalar as inflaton and thermal relic dark matter,” Phys. Rev. D 80, 123507 (2009) [arXiv:0909.0520 [hep-ph]].
[87] S. Kanemura, S. Matsumoto, T. Nabeshima and N. Okada, “Can WIMP Dark Matter overcome the Nightmare Scenario?,” Phys. Rev. D 82, 055026 (2010) [arXiv:1005.5651 [hep-ph]].
[88] J. M. Cline, K. Kainulainen, P. Scott and C. Weniger, “Update on scalar singlet dark matter,” Phys. Rev. D 88, 055025 (2013) [erratum: Phys. Rev. D 92, no.3, 039906 (2015)] [arXiv:1306.4710 [hep-ph]].
[89] P. Athron et al. [GAMBIT], “Status of the scalar singlet dark matter model,” Eur. Phys. J. C 77, no.8, 568 (2017) [arXiv:1705.07931 [hep-ph]].
[90] N. G. Deshpande and E. Ma, “Pattern of Symmetry Breaking with Two Higgs Doublets,” Phys. Rev. D 18, 2574 (1978)
[91] R. Barbieri, L. J. Hall and V. S. Rychkov, “Improved naturalness with a heavy Higgs: An Alternative road to LHC physics,” Phys. Rev. D 74, 015007 (2006) [arXiv:hep-ph/0603188 [hep-ph]].
[92] L. Lopez Honorez, E. Nezri, J. F. Oliver and M. H. G. Tytgat, “The Inert Dou- blet Model: An Archetype for Dark Matter,” JCAP 02, 028 (2007) [arXiv:hep- ph/0612275 [hep-ph]].
[93] A. Goudelis, B. Herrmann and O. St˚al, “Dark matter in the Inert Doublet Model after the discovery of a Higgs-like boson at the LHC,” JHEP 09, 106 (2013) [arXiv:1303.3010 [hep-ph]].
[94] 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, 115011 (2016) [arXiv:1605.08520 [hep-ph]].
[95] M. Cirelli, N. Fornengo and A. Strumia, “Minimal dark matter,” Nucl. Phys. B753, 178-194 (2006) [arXiv:hep-ph/0512090 [hep-ph]].
[96] M. Cirelli, A. Strumia and M. Tamburini, “Cosmology and Astrophysics of Minimal Dark Matter,” Nucl. Phys. B 787, 152-175 (2007) [arXiv:0706.4071 [hep-ph]].
[97] P. Fileviez Perez, H. H. Patel, M. J. Ramsey-Musolf and K. Wang, “Triplet Scalars and Dark Matter at the LHC,” Phys. Rev. D 79, 055024 (2009) [arXiv:0811.3957 [hep-ph]].
[98] A. Pich and P. Tuzon, “Yukawa Alignment in the Two-Higgs-Doublet Model,” Phys. Rev. D 80, 091702 (2009) [arXiv:0908.1554 [hep-ph]].
[99] A. M. Sirunyan et al. [CMS], “Combined measurements of Higgs boson couplings in proton–proton collisions at s = 13 TeV,” Eur. Phys. J. C 79, no.5, 421 (2019) [arXiv:1809.10733 [hep-ex]].
[100] G. Aad et al. [ATLAS], “Combined measurements of Higgs boson production and de- cay using up to 80 fb−1 of proton-proton collision data at s = 13 TeV collected with the ATLAS experiment,” Phys. Rev. D 101, no.1, 012002 (2020) [arXiv:1909.02845 [hep-ex]].
[101] S. Kanemura, M. Kubota and K. Yagyu, “Aligned CP-violating Higgs sector cancel- ing the electric dipole moment,” JHEP 08, 026 (2020) [arXiv:2004.03943 [hep-ph]].
[102] M. Aiko, S. Kanemura, M. Kikuchi, K. Mawatari, K. Sakurai and K. Yagyu, “Prob- ing extended Higgs sectors by the synergy between direct searches at the LHC and precision tests at future lepton colliders,” Nucl. Phys. B 966, 115375 (2021) [arXiv:2010.15057 [hep-ph]].
[103] S. Kanemura, M. Takeuchi and K. Yagyu, “Probing double-aligned two Higgs dou- blet models at LHC,” [arXiv:2112.13679 [hep-ph]].
[104] S. Kanemura, M. Kubota and K. Yagyu, “Testing aligned CP-violating Higgs sector at future lepton colliders,” JHEP 04, 144 (2021) [arXiv:2101.03702 [hep-ph]].
[105] M. Joyce, T. Prokopec and N. Turok, “Electroweak baryogenesis from a classical force,” Phys. Rev. Lett. 75, 1695-1698 (1995) [erratum: Phys. Rev. Lett. 75, 3375(1995)] [arXiv:hep-ph/9408339 [hep-ph]].
[106] M. Joyce, T. Prokopec and N. Turok, “Nonlocal electroweak baryogenesis. Part 1: Thin wall regime,” Phys. Rev. D 53, 2930-2957 (1996) [arXiv:hep-ph/9410281 [hep- ph]]; “Nonlocal electroweak baryogenesis. Part 2: The Classical regime,” Phys. Rev. D 53, 2958-2980 (1996) [arXiv:hep-ph/9410282 [hep-ph]].
[107] J. M. Cline, M. Joyce and K. Kainulainen, “Supersymmetric electroweak baryoge- nesis,” JHEP 07, 018 (2000) [arXiv:hep-ph/0006119 [hep-ph]].
[108] L. Fromme and S. J. Huber, “Top transport in electroweak baryogenesis,” JHEP 03, 049 (2007) [arXiv:hep-ph/0604159 [hep-ph]].
[109] J. M. Cline and K. Kainulainen, “Electroweak baryogenesis at high bubble wall velocities,” Phys. Rev. D 101, no.6, 063525 (2020) [arXiv:2001.00568 [hep-ph]].
[110] M. Aoki, K. Enomoto, S. Kanemura, in preparation.
[111] S. L. Glashow, “Partial Symmetries of Weak Interactions,” Nucl. Phys. 22, 579-588 (1961).
[112] P. W. Higgs, “Broken symmetries, massless particles and gauge fields,” Phys. Lett. 12, 132-133 (1964); “Broken Symmetries and the Masses of Gauge Bosons,” Phys. Rev. Lett. 13, 508-509 (1964); “Spontaneous Symmetry Breakdown without Mass- less Bosons,” Phys. Rev. 145, 1156-1163 (1966).
[113] F. Englert and R. Brout, “Broken Symmetry and the Mass of Gauge Vector Mesons,” Phys. Rev. Lett. 13, 321-323 (1964)
[114] G. S. Guralnik, C. R. Hagen and T. W. B. Kibble, “Global Conservation Laws and Massless Particles,” Phys. Rev. Lett. 13, 585-587 (1964)
[115] Y. Nambu, “Quasiparticles and Gauge Invariance in the Theory of Superconductiv- ity,” Phys. Rev. 117, 648-663 (1960)
[116] J. Goldstone, “Field Theories with Superconductor Solutions,” Nuovo Cim. 19, 154-164 (1961)
[117] Y. Nambu and G. Jona-Lasinio, “Dynamical Model of Elementary Particles Based on an Analogy with Superconductivity. 1.,” Phys. Rev. 122, 345-358 (1961); “Dy- namical Model of Elementary Particles Based on an Analogy with Superconductiv- ity. 2.,” Phys. Rev. 124, 246-254 (1961).
[118] J. Goldstone, A. Salam and S. Weinberg, “Broken Symmetries,” Phys. Rev. 127, 965-970 (1962)
[119] H. Watanabe and H. Murayama, “Unified Description of Nambu-Goldstone Bosons without Lorentz Invariance,” Phys. Rev. Lett. 108, 251602 (2012) [arXiv:1203.0609 [hep-th]].
[120] Y. Hidaka, “Counting rule for Nambu-Goldstone modes in nonrelativistic systems,” Phys. Rev. Lett. 110, no.9, 091601 (2013) [arXiv:1203.1494 [hep-th]].
[121] See, for example, S. Weinberg, “Quantum theory of fields II”, Cambridge University Press.
[122] See, for example, R. N. Mohapatra, P. B. Pal, “Massive neutrinos in physics and astrophysics”, World Scientific.
[123] N. Cabibbo, “Unitary Symmetry and Leptonic Decays,” Phys. Rev. Lett. 10, 531- 533 (1963)
[124] M. Kobayashi and T. Maskawa, “CP Violation in the Renormalizable Theory of Weak Interaction,” Prog. Theor. Phys. 49, 652-657 (1973)
[125] S. L. Glashow, J. Iliopoulos and L. Maiani, “Weak Interactions with Lepton-Hadron Symmetry,” Phys. Rev. D 2, 1285-1292 (1970)
[126] C. Jarlskog, “A Basis Independent Formulation of the Connection Between Quark Mass Matrices, CP Violation and Experiment,” Z. Phys. C 29, 491-497 (1985); “Commutator of the Quark Mass Matrices in the Standard Electroweak Model and a Measure of Maximal CP Violation,” Phys. Rev. Lett. 55, 1039 (1985).
[127] P. H. Frampton and C. Jarlskog, “Systematics of Quark Mass Matrices in the Stan- dard Electroweak Model,” Phys. Lett. B 154, 421-424 (1985)
[128] A. E. Nelson, D. B. Kaplan and A. G. Cohen, Nucl. Phys. B 373, 453-478 (1992) doi:10.1016/0550-3213(92)90440-M
[129] K. Funakubo, “CP violation and baryogenesis at the electroweak phase transition,” Prog. Theor. Phys. 96, 475-520 (1996) [arXiv:hep-ph/9608358 [hep-ph]].
[130] G. R. Farrar and M. E. Shaposhnikov, Phys. Rev. Lett. 70, 2833-2836 (1993) [erra- tum: Phys. Rev. Lett. 71, 210 (1993)] [arXiv:hep-ph/9305274 [hep-ph]]; Phys. Rev. D 50, 774 (1994) [arXiv:hep-ph/9305275 [hep-ph]].
[131] D. A. Kirzhnits and A. D. Linde, “Macroscopic Consequences of the Weinberg Model,” Phys. Lett. B 42, 471-474 (1972)
[132] L. Dolan and R. Jackiw, “Symmetry Behavior at Finite Temperature,” Phys. Rev. D 9, 3320-3341 (1974)
[133] S. Weinberg, “Gauge and Global Symmetries at High Temperature,” Phys. Rev. D9, 3357-3378 (1974)
[134] M. E. Carrington, “The Effective potential at finite temperature in the Standard Model,” Phys. Rev. D 45, 2933-2944 (1992)
[135] P. Meade and H. Ramani, “Unrestored Electroweak Symmetry,” Phys. Rev. Lett.122, no.4, 041802 (2019) [arXiv:1807.07578 [hep-ph]].
[136] I. Baldes and G. Servant, “High scale electroweak phase transition: baryogenesis\& symmetry non-restoration,” JHEP 10, 053 (2018) [arXiv:1807.08770 [hep-ph]].
[137] M. Carena, C. Krause, Z. Liu and Y. Wang, “New approach to electroweak sym- metry nonrestoration,” Phys. Rev. D 104, no.5, 055016 (2021) [arXiv:2104.00638 [hep-ph]].
[138] W. Chao, H. K. Guo and X. F. Li, “First Order Color Symmetry Break- ing and Restoration Triggered by Electroweak Symmetry Non-restoration,” [arXiv:2112.13580 [hep-ph]].
[139] M. Dine, R. G. Leigh, P. Y. Huet, A. D. Linde and D. A. Linde, “Towards the theory of the electroweak phase transition,” Phys. Rev. D 46, 550-571 (1992) [arXiv:hep- ph/9203203 [hep-ph]].
[140] S. Kanemura, S. Kiyoura, Y. Okada, E. Senaha and C. P. Yuan, “New physics effect on the Higgs selfcoupling,” Phys. Lett. B 558, 157-164 (2003) [arXiv:hep- ph/0211308 [hep-ph]].
[141] S. Kanemura, Y. Okada, E. Senaha and C. P. Yuan, “Higgs coupling constants as a probe of new physics,” Phys. Rev. D 70, 115002 (2004) [arXiv:hep-ph/0408364 [hep-ph]].
[142] J. Braathen and S. Kanemura, “On two-loop corrections to the Higgs trilinear cou- pling in models with extended scalar sectors,” Phys. Lett. B 796, 38-46 (2019) [arXiv:1903.05417 [hep-ph]]; “Leading two-loop corrections to the Higgs boson self- couplings in models with extended scalar sectors,” Eur. Phys. J. C 80, no.3, 227 (2020) [arXiv:1911.11507 [hep-ph]].
[143] S. Kanemura, Y. Okada and E. Senaha, “Electroweak baryogenesis and quantum corrections to the triple Higgs boson coupling,” Phys. Lett. B 606, 361-366 (2005) [arXiv:hep-ph/0411354 [hep-ph]].
[144] J. M. Cline and K. Kainulainen, “A New source for electroweak baryogenesis in the MSSM,” Phys. Rev. Lett. 85, 5519-5522 (2000) [arXiv:hep-ph/0002272 [hep-ph]].
[145] G. D. Moore, “Sphaleron rate in the symmetric electroweak phase,” Phys. Rev. D62, 085011 (2000) [arXiv:hep-ph/0001216 [hep-ph]].
[146] B. Pontecorvo, “Mesonium and anti-mesonium,” Sov. Phys. JETP 6, 429 (1957); “Inverse beta processes and nonconservation of lepton charge,” Zh. Eksp. Teor. Fiz. 34, 247 (1957); “Neutrino Experiments and the Problem of Conservation of Leptonic Charge,” Zh. Eksp. Teor. Fiz. 53, 1717-1725 (1967).
[147] Z. Maki, M. Nakagawa and S. Sakata, “Remarks on the unified model of elementary particles,” Prog. Theor. Phys. 28, 870-880 (1962).
[148] S. M. Bilenky and S. T. Petcov, “Massive Neutrinos and Neutrino Oscillations,” Rev. Mod. Phys. 59, 671 (1987) [erratum: Rev. Mod. Phys. 61, 169 (1989); erratum:Rev. Mod. Phys. 60, 575-575 (1988)].
[149] A. Gando et al. [KamLAND-Zen], “Search for Majorana Neutrinos near the Inverted Mass Hierarchy Region with KamLAND-Zen,” Phys. Rev. Lett. 117, no.8, 082503 (2016) [arXiv:1605.02889 [hep-ex]].
[150] P. Sikivie, L. Susskind, M. B. Voloshin and V. I. Zakharov, “Isospin Breaking in Technicolor Models,” Nucl. Phys. B 173, 189-207 (1980)
[151] H. E. Haber and A. Pomarol, “Constraints from global symmetries on radiative corrections to the Higgs sector,” Phys. Lett. B 302, 435-441 (1993) [arXiv:hep- ph/9207267 [hep-ph]].
[152] A. Pomarol and R. Vega, “Constraints on CP violation in the Higgs sector from the rho parameter,” Nucl. Phys. B 413, 3-15 (1994) [arXiv:hep-ph/9305272 [hep-ph]].
[153] J. M. Gerard and M. Herquet, “A Twisted custodial symmetry in the two-Higgs- doublet model,” Phys. Rev. Lett. 98, 251802 (2007) [arXiv:hep-ph/0703051 [hep- ph]].
[154] H. E. Haber and D. O’Neil, “Basis-independent methods for the two-Higgs-doublet model III: The CP-conserving limit, custodial symmetry, and the oblique parameters S, T, U,” Phys. Rev. D 83, 055017 (2011) [arXiv:1011.6188 [hep-ph]].
[155] B. Grzadkowski, M. Maniatis and J. Wudka, “The bilinear formalism and the custodial symmetry in the two-Higgs-doublet model,” JHEP 11, 030 (2011) [arXiv:1011.5228 [hep-ph]].
[156] M. Aiko and S. Kanemura, “New scenario for aligned Higgs couplings originated from the twisted custodial symmetry at high energies,” JHEP 02, 046 (2021) [arXiv:2009.04330 [hep-ph]].
[157] S. Kanemura, T. Kasai, G. L. Lin, Y. Okada, J. J. Tseng and C. P. Yuan, “Phe- nomenology of Higgs bosons in the Zee model,” Phys. Rev. D 64, 053007 (2001) [arXiv:hep-ph/0011357 [hep-ph]].
[158] L. Wolfenstein, “A Theoretical Pattern for Neutrino Oscillations,” Nucl. Phys. B175, 93-96 (1980)
[159] V. D. Barger, J. L. Hewett and R. J. N. Phillips, “New Constraints on the Charged Higgs Sector in Two Higgs Doublet Models,” Phys. Rev. D 41, 3421-3441 (1990)
[160] Y. Grossman, “Phenomenology of models with more than two Higgs doublets,” Nucl. Phys. B 426, 355-384 (1994) [arXiv:hep-ph/9401311 [hep-ph]].
[161] M. Aoki, S. Kanemura, K. Tsumura and K. Yagyu, “Models of Yukawa interaction in the two Higgs doublet model, and their collider phenomenology,” Phys. Rev. D 80, 015017 (2009) [arXiv:0902.4665 [hep-ph]].
[162] K. Cheung and O. Seto, “Phenomenology of TeV right-handed neutrino and the dark matter model,” Phys. Rev. D 69, 113009 (2004) [arXiv:hep-ph/0403003 [hep- ph]].
[163] F. Zwicky, “Die Rotverschiebung von extragalaktischen Nebeln,” Helv. Phys. Acta6, 110-127 (1933)
[164] E. Kolb, M. Turner, “The Early Universe”, CRC press.
[165] S. Davidson and H. E. Haber, “Basis-independent methods for the two-Higgs- doublet model,” Phys. Rev. D 72, 035004 (2005) [erratum: Phys. Rev. D 72, 099902(2005)] [arXiv:hep-ph/0504050 [hep-ph]].
[166] A. G. Akeroyd, M. Aoki, A. Arhrib, L. Basso, I. F. Ginzburg, R. Guedes,J. Hernandez-Sanchez, K. Huitu, T. Hurth and M. Kadastik, et al. “Prospects for charged Higgs searches at the LHC,” Eur. Phys. J. C 77, no.5, 276 (2017) [arXiv:1607.01320 [hep-ph]].
[167] A. Arbey, F. Mahmoudi, O. Stal and T. Stefaniak, “Status of the Charged Higgs Boson in Two Higgs Doublet Models,” Eur. Phys. J. C 78, no.3, 182 (2018) [arXiv:1706.07414 [hep-ph]].
[168] G. Abbiendi et al. [ALEPH, DELPHI, L3, OPAL and LEP], “Search for Charged Higgs bosons: Combined Results Using LEP Data,” Eur. Phys. J. C 73, 2463 (2013) [arXiv:1301.6065 [hep-ex]].
[169] D. de Florian et al. [LHC HiAiggs Cross Section Working Group], “Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector,” [arXiv:1610.07922 [hep-ph]].
[170] A. M. Sirunyan et al. [CMS], “Search for cha√rged Higgs bosons in the H± → τ ±ντdecay channel in proton-proton collisions at s = 13 TeV,” JHEP 07, 142 (2019)[arXiv:1903.04560 [hep-ex]].
[171] G. Aad et al. [ATLAS], “Search for charged Higgs bosons decaying into a top quark and a bottom quark at s = 13 TeV with the ATLAS detector,” JHEP 06, 145 (2021) [arXiv:2102.10076 [hep-ex]].
[172] M. Aaboud et al. [ATLAS], “Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton–proton collisions at s = 13 TeV with the ATLAS detector,” Eur. Phys. J. C 78, no.7, 565 (2018) [arXiv:1804.10823 [hep-ex]].
[173] G. Aad et al. [ATLAS], “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, 051801 (2020) [arXiv:2002.12223 [hep-ex]].
[174] T. Enomoto and R. Watanabe, “Flavor constraints on the Two Higgs Doublet Mod- els of Z2 symmetric and aligned types,” JHEP 05, 002 (2016) [arXiv:1511.05066 [hep-ph]].
[175] J. Haller, A. Hoecker, R. Kogler, K. M¨onig, T. Peiffer and J. Stelzer, “Update of the global electroweak fit and constraints on two-Higgs-doublet models,” Eur. Phys.J. C 78, no.8, 675 (2018) [arXiv:1803.01853 [hep-ph]].
[176] V. Khachatryan et al. [CMS and LHCb], “Observation of the rare B0 → µ+µ−decay from the combined analysis of CMS and LHCb data,” Nature 522, 68-72 (2015) [arXiv:1411.4413 [hep-ex]].
[177] R. Aaij et al. [LHCb], “Measurement of the B0 → µ+µ− branching fraction and effective lifetime and search for B0 µ+µ− decays,” Phys. Rev. Lett. 118, no.19,191801 (2017) [arXiv:1703.05747 [hep-ex]].
[178] V. Andreev et al. [ACME], “Improved limit on the electric dipole moment of the electron,” Nature 562, no.7727, 355-360 (2018)
[179] M. Jung and A. Pich, “Electric Dipole Moments in Two-Higgs-Doublet Models,” JHEP 04, 076 (2014) [arXiv:1308.6283 [hep-ph]].
[180] K. Cheung, J. S. Lee, E. Senaha and P. Y. Tseng, “Confronting Higgcision with Electric Dipole Moments,” JHEP 06, 149 (2014) [arXiv:1403.4775 [hep-ph]].
[181] S. M. Barr and A. Zee, “Electric Dipole Moment of the Electron and of the Neutron,” Phys. Rev. Lett. 65, 21-24 (1990) [erratum: Phys. Rev. Lett. 65, 2920 (1990)]
[182] C. Abel et al. [nEDM], “Measurement of the permanent electric dipole moment of the neutron,” Phys. Rev. Lett. 124, no.8, 081803 (2020) [arXiv:2001.11966 [hep-ex]].
[183] M. Pospelov and A. Ritz, “Neutron EDM from electric and chromoelectric dipole moments of quarks,” Phys. Rev. D 63, 073015 (2001) [arXiv:hep-ph/0010037 [hep- ph]].
[184] J. Hisano, J. Y. Lee, N. Nagata and Y. Shimizu, “Reevaluation of Neutron Elec- tric Dipole Moment with QCD Sum Rules,” Phys. Rev. D 85, 114044 (2012) [arXiv:1204.2653 [hep-ph]].
[185] K. Fuyuto, J. Hisano, N. Nagata and K. Tsumura, “QCD Corrections to Quark (Chromo)Electric Dipole Moments in High-scale Supersymmetry,” JHEP 12, 010 (2013) [arXiv:1308.6493 [hep-ph]].
[186] T. Abe, J. Hisano, T. Kitahara and K. Tobioka, “Gauge invariant Barr-Zee type contributions to fermionic EDMs in the two-Higgs doublet models,” JHEP 01, 106 (2014) [erratum: JHEP 04, 161 (2016)] [arXiv:1311.4704 [hep-ph]].
[187] S. Weinberg, “Larger Higgs Exchange Terms in the Neutron Electric Dipole Mo- ment,” Phys. Rev. Lett. 63, 2333 (1989)
[188] D. A. Dicus, “Neutron Electric Dipole Moment From Charged Higgs Exchange,” Phys. Rev. D 41, 999 (1990)
[189] V. M. Khatsimovsky, I. B. Khriplovich and A. S. Yelkhovsky, “Neutron Electric Dipole Moment, T Odd Nuclear Forces and Nature of CP Violation,” Annals Phys. 186, 1-14 (1988)
[190] M. E. Peskin and T. Takeuchi, “A New constraint on a strongly interacting Higgs sector,” Phys. Rev. Lett. 65, 964-967 (1990); “Estimation of oblique electroweak corrections,” Phys. Rev. D 46, 381-409 (1992).
[191] S. Kanemura, T. Kubota and E. Takasugi, “Lee-Quigg-Thacker bounds for Higgs bo- son masses in a two doublet model,” Phys. Lett. B 313, 155-160 (1993) [arXiv:hep- ph/9303263 [hep-ph]].
[192] A. G. Akeroyd, A. Arhrib and E. M. Naimi, “Note on tree level unitarity in the general two Higgs doublet model,” Phys. Lett. B 490, 119-124 (2000) [arXiv:hep- ph/0006035 [hep-ph]].
[193] I. F. Ginzburg and I. P. Ivanov, “Tree-level unitarity constraints in the most general 2HDM,” Phys. Rev. D 72, 115010 (2005) [arXiv:hep-ph/0508020 [hep-ph]].
[194] S. Kanemura and K. Yagyu, “Unitarity bound in the most general two Higgs doublet model,” Phys. Lett. B 751, 289-296 (2015) [arXiv:1509.06060 [hep-ph]].
[195] S. Nie and M. Sher, “Vacuum stability bounds in the two Higgs doublet model,” Phys. Lett. B 449, 89-92 (1999) [arXiv:hep-ph/9811234 [hep-ph]].
[196] S. Kanemura, T. Kasai and Y. Okada, “Mass bounds of the lightest CP even Higgs boson in the two Higgs doublet model,” Phys. Lett. B 471, 182-190 (1999) [arXiv:hep-ph/9903289 [hep-ph]].
[197] P. M. Ferreira, R. Santos and A. Barroso, “Stability of the tree-level vacuum in two Higgs doublet models against charge or CP spontaneous violation,” Phys. Lett. B 603, 219-229 (2004) [erratum: Phys. Lett. B 629, 114-114 (2005)] [arXiv:hep-ph/0406231 [hep-ph]].
[198] S. R. Coleman and E. J. Weinberg, “Radiative Corrections as the Origin of Spon- taneous Symmetry Breaking,” Phys. Rev. D 7, 1888-1910 (1973)
[199] S. Baum, M. Carena, N. R. Shah, C. E. M. Wagner and Y. Wang, “Nucleation is more than critical: A case study of the electroweak phase transition in the NMSSM,” JHEP 03, 055 (2021) [arXiv:2009.10743 [hep-ph]].
[200] R. R. Parwani, “Resummation in a hot scalar field theory,” Phys. Rev. D 45, 4695 (1992) [erratum: Phys. Rev. D 48, 5965 (1993)] [arXiv:hep-ph/9204216 [hep-ph]].
[201] L. D. McLerran, E. Mottola and M. E. Shaposhnikov, “Sphalerons and Axion Dy- namics in High Temperature QCD,” Phys. Rev. D 43, 2027-2035 (1991)
[202] G. F. Giudice and M. E. Shaposhnikov, “Strong sphalerons and electroweak baryo- genesis,” Phys. Lett. B 326, 118-124 (1994) [arXiv:hep-ph/9311367 [hep-ph]].
[203] C. L. Wainwright, “CosmoTransitions: Computing Cosmological Phase Transition Temperatures and Bubble Profiles with Multiple Fields,” Comput. Phys. Commun. 183, 2006-2013 (2012) [arXiv:1109.4189 [hep-ph]].
[204] G. D. Moore, “Computing the strong sphaleron rate,” Phys. Lett. B 412, 359-370 (1997) [arXiv:hep-ph/9705248 [hep-ph]].
[205] P. Huet and A. E. Nelson, “Electroweak baryogenesis in supersymmetric models,” Phys. Rev. D 53, 4578-4597 (1996) [arXiv:hep-ph/9506477 [hep-ph]].
[206] J. M. Cline and B. Laurent, “Electroweak baryogenesis from light fermion sources: A critical study,” Phys. Rev. D 104, no.8, 083507 (2021) [arXiv:2108.04249 [hep- ph]].
[207] M. Cepeda, S. Gori, P. Ilten, M. Kado, F. Riva, R. Abdul Khalek, A. Aboubrahim,J. Alimena, S. Alioli and A. Alves, et al. “Report from Working Group 2: Higgs Physics at the HL-LHC and HE-LHC,” CERN Yellow Rep. Monogr. 7, 221-584 (2019) [arXiv:1902.00134 [hep-ph]].
[208] K. Fujii, C. Grojean, M. E. Peskin, T. Barklow, Y. Gao, S. Kanemura, H. D. Kim,J. List, M. Nojiri and M. Perelstein, et al. “Physics Case for the International Linear Collider,” [arXiv:1506.05992 [hep-ex]].
[209] P. Bambade, T. Barklow, T. Behnke, M. Berggren, J. Brau, P. Burrows, D. Denisov,A. Faus-Golfe, B. Foster and K. Fujii, et al. “The International Linear Collider: A Global Project,” [arXiv:1903.01629 [hep-ex]].
[210] P. N. Burrows et al. [CLICdp and CLIC], “The Compact Linear Collider (CLIC) - 2018 Summary Report,” [arXiv:1812.06018 [physics.acc-ph]].
[211] J. W. Martin, “Current status of neutron electric dipole moment experiments,” J. Phys. Conf. Ser. 1643, no.1, 012002 (2020)
[212] D. J. H. Chung, B. Garbrecht, M. J. Ramsey-Musolf and S. Tulin, “Lepton-mediated electroweak baryogenesis,” Phys. Rev. D 81, 063506 (2010) [arXiv:0905.4509 [hep- ph]].
[213] J. De Vries, M. Postma and J. van de Vis, “The role of leptons in electroweak baryogenesis,” JHEP 04, 024 (2019) [arXiv:1811.11104 [hep-ph]].
[214] K. P. Xie, “Lepton-mediated electroweak baryogenesis, gravitational waves and the 4τ final state at the collider,” JHEP 02, 090 (2021) [arXiv:2011.04821 [hep-ph]].
[215] K. Enomoto, S. Kanemura and Y. Mura, work in progress.
[216] A. Riotto, “Towards a nonequilibrium quantum field theory approach to electroweak baryogenesis,” Phys. Rev. D 53, 5834-5841 (1996) [arXiv:hep-ph/9510271 [hep- ph]]; “Supersymmetric electroweak baryogenesis, nonequilibrium field theory and quantum Boltzmann equations,” Nucl. Phys. B 518, 339-360 (1998) [arXiv:hep- ph/9712221 [hep-ph]].
[217] E. Kou et al. [Belle-II], “The Belle II Physics Book,” PTEP 2019, no.12, 123C01 (2019) [erratum: PTEP 2020, no.2, 029201 (2020)] [arXiv:1808.10567 [hep-ex]].
[218] R. Aaij et al. [LHCb], “Implications of LHCb measurements and future prospects,” Eur. Phys. J. C 73, no.4, 2373 (2013) [arXiv:1208.3355 [hep-ex]].
[219] M. Benzke, S. J. Lee, M. Neubert and G. Paz, “Long-Distance Dominance of the CP Asymmetry in B Xs,d + γ Decays,” Phys. Rev. Lett. 106, 141801 (2011) [arXiv:1012.3167 [hep-ph]].
[220] S. Watanuki et al. [Belle], “Measurements of isospin asymmetry and difference of direct CP asymmetries in inclusive B Xsγ decays,” Phys. Rev. D 99, no.3, 032012 (2019) [arXiv:1807.04236 [hep-ex]].
[221] D. Jeans and G. W. Wilson, “Measuring the CP state of tau lepton pairs from Higgs decay at the ILC,” Phys. Rev. D 98, no.1, 013007 (2018) [arXiv:1804.01241 [hep-ex]].
[222] O. J. P. Eboli, G. C. Marques, S. F. Novaes and A. A. Natale, “TWIN HIGGS BOSON PRODUCTION,” Phys. Lett. B 197, 269-272 (1987)
[223] D. A. Dicus, C. Kao and S. S. D. Willenbrock, “Higgs Boson Pair Production From Gluon Fusion,” Phys. Lett. B 203, 457-461 (1988)
[224] E. W. N. Glover and J. J. van der Bij, “HIGGS BOSON PAIR PRODUCTION VIA GLUON FUSION,” Nucl. Phys. B 309, 282-294 (1988)
[225] T. Plehn, M. Spira and P. M. Zerwas, “Pair production of neutral Higgs particles in gluon-gluon collisions,” Nucl. Phys. B 479, 46-64 (1996) [erratum: Nucl. Phys. B 531, 655-655 (1998)] [arXiv:hep-ph/9603205 [hep-ph]].
[226] A. Djouadi, W. Kilian, M. Muhlleitner and P. M. Zerwas, “Production of neutral Higgs boson pairs at LHC,” Eur. Phys. J. C 10, 45-49 (1999) [arXiv:hep-ph/9904287 [hep-ph]].
[227] X. Li and M. B. Voloshin, “Remarks on double Higgs boson production by gluon fusion at threshold,” Phys. Rev. D 89, no.1, 013012 (2014) [arXiv:1311.5156 [hep- ph]].
[228] D. Gon¸calves, T. Han, F. Kling, T. Plehn and M. Takeuchi, “Higgs boson pair production at future hadron colliders: From kinematics to dynamics,” Phys. Rev. D 97, no.11, 113004 (2018) [arXiv:1802.04319 [hep-ph]].
[229] E. Asakawa, D. Harada, S. Kanemura, Y. Okada and K. Tsumura, “Higgs boson pair production in new physics models at hadron, lepton, and photon colliders,” Phys. Rev. D 82, 115002 (2010) [arXiv:1009.4670 [hep-ph]].
[230] R. Apreda, M. Maggiore, A. Nicolis and A. Riotto, “Gravitational waves from elec- troweak phase transitions,” Nucl. Phys. B 631, 342-368 (2002) [arXiv:gr-qc/0107033 [gr-qc]].
[231] C. Grojean and G. Servant, “Gravitational Waves from Phase Transitions at the Electroweak Scale and Beyond,” Phys. Rev. D 75, 043507 (2007) [arXiv:hep- ph/0607107 [hep-ph]].
[232] M. Kakizaki, S. Kanemura and T. Matsui, “Gravitational waves as a probe of extended scalar sectors with the first order electroweak phase transition,” Phys. Rev. D 92, no.11, 115007 (2015) [arXiv:1509.08394 [hep-ph]].
[233] P. Amaro-Seoane et al. [LISA], “Laser Interferometer Space Antenna,” [arXiv:1702.00786 [astro-ph.IM]].
[234] N. Seto, S. Kawamura and T. Nakamura, “Possibility of direct measurement of the acceleration of the universe using 0.1-Hz band laser interferometer gravitational wave antenna in space,” Phys. Rev. Lett. 87, 221103 (2001) [arXiv:astro-ph/0108011 [astro-ph]].
[235] V. Corbin and N. J. Cornish, “Detecting the cosmic gravitational wave background with the big bang observer,” Class. Quant. Grav. 23, 2435-2446 (2006) [arXiv:gr- qc/0512039 [gr-qc]].
[236] G. Aad et al. [ATLAS], “Searches for electroweak production of supersymmetric particles with compressed mass spectra in s = 13 TeV pp collisions with the ATLAS detector,” Phys. Rev. D 101, no.5, 052005 (2020) [arXiv:1911.12606 [hep- ex]].
[237] G. Aad et al. [ATLAS], “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in s = 13 TeV pp collisions using the ATLAS detector,” Eur. Phys. J. C 80, no.2,123 (2020) [arXiv:1908.08215 [hep-ex]].
[238] G. Aad et al. [ATLAS], “Search for direct stau production in events with two hadronic τ -leptons in s = 13 TeV pp collisions with the ATLAS detector,” Phys. Rev. D 101, no.3, 032009 (2020) [arXiv:1911.06660 [hep-ex]].
[239] A. M. Baldini et al. [MEG], “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, 434 (2016) [arXiv:1605.05081 [hep-ex]].
[240] B. Aubert et al. [BaBar], “Searches for Lepton Flavor Violation in the Decays tau+- e+- gamma and tau+- mu+- gamma,” Phys. Rev. Lett. 104, 021802 (2010)[arXiv:0908.2381 [hep-ex]].
[241] U. Bellgardt et al. [SINDRUM], “Search for the Decay mu+ e+ e+ e-,” Nucl. Phys. B 299, 1-6 (1988)
[242] K. Hayasaka, K. Inami, Y. Miyazaki, K. Arinstein, V. Aulchenko, T. Aushev,A. M. Bakich, A. Bay, K. Belous and V. Bhardwaj, et al. “Search for Lepton Flavor Violating Tau Decays into Three Leptons with 719 Million Produced Tau+Tau- Pairs,” Phys. Lett. B 687, 139-143 (2010) [arXiv:1001.3221 [hep-ex]].
[243] A. M. Sirunyan et al. [CMS], “Search for lepton flavour violating decays of the Higgs boson to µτ and eτ in proton-proton collisions at s = 13 TeV,” JHEP 06, 001 (2018) [arXiv:1712.07173 [hep-ex]].
[244] V. Khachatryan et al. [CMS], “Search for lepton flavour violating decays of the Higgs boson to eτ and eµ in proton–proton collisions at s = 8 TeV,” Phys. Lett. B 763, 472-500 (2016) [arXiv:1607.03561 [hep-ex]].
[245] W. H. Bertl et al. [SINDRUM II], “A Search for muon to electron conversion in muonic gold,” Eur. Phys. J. C 47, 337-346 (2006)
[246] M. Aoki, S. Kanemura, K. Sakurai and H. Sugiyama, “Testing neutrino mass gener- ation mechanisms from the lepton flavor violating decay of the Higgs boson,” Phys. Lett. B 763, 352-357 (2016) [arXiv:1607.08548 [hep-ph]].
[247] M. Aoki, S. Kanemura and K. Yagyu, “Triviality and vacuum stability bounds in the three-loop neutrino mass model,” Phys. Rev. D 83, 075016 (2011) [arXiv:1102.3412 [hep-ph]].
[248] G. Passarino and M. J. G. Veltman, “One Loop Corrections for e+ e- Annihilation Into mu+ mu- in the Weinberg Model,” Nucl. Phys. B 160, 151-207 (1979)
[249] M. Srednicki, R. Watkins and K. A. Olive, “Calculations of Relic Densities in the Early Universe,” Nucl. Phys. B 310, 693 (1988)
[250] P. Gondolo and G. Gelmini, “Cosmic abundances of stable particles: Improved analysis,” Nucl. Phys. B 360, 145-179 (1991)
[251] H. Y. Cheng and C. W. Chiang, “Revisiting Scalar and Pseudoscalar Couplings with Nucleons,” JHEP 07, 009 (2012) [arXiv:1202.1292 [hep-ph]].
[252] E. Aprile et al. [XENON], “Dark Matter Search Results from a One Ton-Year Expo- sure of XENON1T,” Phys. Rev. Lett. 121, no.11, 111302 (2018) [arXiv:1805.12562[astro-ph.CO]].
[253] A. M. Baldini et al. [MEG II], “The design of the MEG II experiment,” Eur. Phys.J. C 78, no.5, 380 (2018) [arXiv:1801.04688 [physics.ins-det]].
[254] A. Blondel, A. Bravar, M. Pohl, S. Bachmann, N. Berger, M. Kiehn, A. Schon- ing, D. Wiedner, B. Windelband and P. Eckert, et al. “Research Proposal for an Experiment to Search for the Decay µ → eee,” [arXiv:1301.6113 [physics.ins-det]].
[255] K. Arndt et al. [Mu3e], “Technical design of the phase I Mu3e experiment,” Nucl. Instrum. Meth. A 1014, 165679 (2021) [arXiv:2009.11690 [physics.ins-det]].
[256] K. Abe et al. [Hyper-Kamiokande], “Hyper-Kamiokande Design Report,” [arXiv:1805.04163 [physics.ins-det]].
[257] D. S. Akerib et al. [LZ], “LUX-ZEPLIN (LZ) Conceptual Design Report,” [arXiv:1509.02910 [physics.ins-det]].
[258] J. Aalbers et al. [DARWIN], “DARWIN: towards the ultimate dark matter detec- tor,” JCAP 11, 017 (2016) [arXiv:1606.07001 [astro-ph.IM]].
[259] J. R. Espinosa, M. Quiros and F. Zwirner, “On the nature of the electroweak phase transition,” Phys. Lett. B 314, 206-216 (1993) [arXiv:hep-ph/9212248 [hep-ph]].
論文の公開元へ
