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Phase transitions, anomalous baryon number violation, and electroweak multiplet dark matter

Yanda Wu1,2,*, Wenxing Zhang3,4,5,†, and Michael J. Ramsey-Musolf1,2,6,7,‡

  • *Contact author: yanda.wu7@sjtu.edu.cn
  • †Contact author: zhangwenxing@hbu.edu.cn
  • ‡Contact author: mjrm@sjtu.edu.cn, mjrm@physics.umass.edu

Phys. Rev. D 112, 053003 – Published 12 September, 2025

DOI: https://doi.org/10.1103/lz6d-kn77

Abstract

We perform a comprehensive analysis of baryon number violation during an electroweak phase transition (EWPT) within the framework of a scalar electroweak multiplet extension of the Standard Model (SM). We classify the multiplet representations, topological properties, and corresponding thermal histories. Sphaleron or monopole topological field solutions emerge during the EWPT depending on the stage of the phase transition and the hypercharge of the new scalar multiplet. Furthermore, the monopole field solution pertains when the neutral component of the additional scalar multiplet is a viable dark matter candidate. We further analyze other formal considerations, including the construction of the “sphaleron matrix” for higher dimensional representations, computation of the sphaleron and monopole masses, and the choice of boundary conditions when solving the field equations of motion. We apply these considerations to the computation of sphaleron energy and monopole mass within the context of a multistep EWPT, employing the SU(2)L septuplet scalar extension to the SM as a case of study from the minimal dark matter paradigm. For the first step of a two-step EWPT, we delineate the relationship between the monopole mass and the parameters relevant to dark matter phenomenology.

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References (64)

  1. A. D. Sakharov, Violation of CP Invariance, C asymmetry, and baryon asymmetry of the universe, Pis’ma Zh. Eksp. Teor. Fiz. 5, 32 (1967).
  2. M. B. Gavela, P. Hernandez, J. Orloff, and O. Pene, Standard model CP violation and baryon asymmetry, Mod. Phys. Lett. A 9, 795 (1994).
  3. P. Huet and E. Sather, Electroweak baryogenesis and Standard Model CP violation, Phys. Rev. D 51, 379 (1995).
  4. M. B. Gavela, P. Hernandez, J. Orloff, O. Pene, and C. Quimbay, Standard model CP violation and baryon asymmetry. Part 2: Finite temperature, Nucl. Phys. B430, 382 (1994).
  5. 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 (1996).
  6. M. Gurtler, E.-M. Ilgenfritz, and A. Schiller, Where the electroweak phase transition ends, Phys. Rev. D 56, 3888 (1997).
  7. M. Laine and K. Rummukainen, What’s new with the electroweak phase transition?, Nucl. Phys. B, Proc. Suppl. 73, 180 (1999).
  8. F. Csikor, Z. Fodor, and J. Heitger, Endpoint of the hot electroweak phase transition, Phys. Rev. Lett. 82, 21 (1999).
  9. Y. Aoki, F. Csikor, Z. Fodor, and A. Ukawa, The endpoint of the first order phase transition of the SU(2) gauge Higgs model on a four-dimensional isotropic lattice, Phys. Rev. D 60, 013001 (1999).
  10. D. E. Morrissey and M. J. Ramsey-Musolf, Electroweak baryogenesis, New J. Phys. 14, 125003 (2012).
  11. M. J. Ramsey-Musolf, The electroweak phase transition: A collider target, J. High Energy Phys. 09 (2020) 179.
  12. D. Bodeker and W. Buchmuller, Baryogenesis from the weak scale to the grand unification scale, Rev. Mod. Phys. 93, 035004 (2021).
  13. V. A. Kuzmin, V. A. Rubakov, and M. E. Shaposhnikov, On the anomalous electroweak baryon number nonconservation in the early universe, Phys. Lett. 155B, 36 (1985).
  14. V. A. Rubakov and M. E. Shaposhnikov, Electroweak baryon number nonconservation in the early universe and in high-energy collisions, Usp. Fiz. Nauk 166, 493 (1996).
  15. H. H. Patel and M. J. Ramsey-Musolf, Baryon washout, electroweak phase transition, and perturbation theory, J. High Energy Phys. 07 (2011) 029.
  16. P. B. Arnold and L. D. McLerran, Sphalerons, small fluctuations and baryon number violation in electroweak theory, Phys. Rev. D 36, 581 (1987).
  17. L. Carson, X. Li, L. D. McLerran, and R.-T. Wang, Exact computation of the small fluctuation determinant around a sphaleron, Phys. Rev. D 42, 2127 (1990).
  18. J. Baacke and S. Junker, Quantum fluctuations around the electroweak sphaleron, Phys. Rev. D 49, 2055 (1994).
  19. H. Georgi and M. Machacek, Doubly charged Higgs bosons, Nucl. Phys. B262, 463 (1985).
  20. H. H. Patel and M. J. Ramsey-Musolf, Stepping into electroweak symmetry breaking: Phase transitions and Higgs phenomenology, Phys. Rev. D 88, 035013 (2013).
  21. N. Blinov, J. Kozaczuk, D. E. Morrissey, and C. Tamarit, Electroweak baryogenesis from exotic electroweak symmetry breaking, Phys. Rev. D 92, 035012 (2015).
  22. L. Niemi, M. J. Ramsey-Musolf, T. V. I. Tenkanen, and D. J. Weir, Thermodynamics of a two-step electroweak phase transition, Phys. Rev. Lett. 126, 171802 (2021).
  23. S. Bottaro, D. Buttazzo, M. Costa, R. Franceschini, P. Panci, D. Redigolo, and L. Vittorio, The last complex WIMPs standing, Eur. Phys. J. C 82, 992 (2022).
  24. P. Panci, Electroweak multiplets as dark matter candidates: A brief review, Proc. Sci., CORFU2023 (2024) 033 [arXiv:2405.05087].
  25. J. Preskill, Magnetic monopoles, Annu. Rev. Nucl. Part. Sci. 34, 461 (1984).
  26. N. S. Manton, Topology in the Weinberg-Salam theory, Phys. Rev. D 28, 2019 (1983).
  27. G. ’t Hooft, Magnetic monopoles in unified gauge theories, Nucl. Phys. B79, 276 (1974).
  28. A. M. Polyakov, Particle spectrum in quantum field theory, JETP Lett. 20, 194 (1974).
  29. F. R. Klinkhamer and R. Laterveer, The sphaleron at finite mixing angle, Z. Phys. C 53, 247 (1992).
  30. A. Ahriche, T. A. Chowdhury, and S. Nasri, Sphalerons and the electroweak phase transition in models with higher scalar representations, J. High Energy Phys. 11 (2014) 096.
  31. R. M. Fonseca, GroupMath: A Mathematica package for group theory calculations, Comput. Phys. Commun. 267, 108085 (2021).
  32. W. Chao, G.-J. Ding, X.-G. He, and M. Ramsey-Musolf, Scalar electroweak multiplet dark matter, J. High Energy Phys. 08 (2019) 058.
  33. S. L. Adler, Axial vector vertex in spinor electrodynamics, Phys. Rev. 177, 2426 (1969).
  34. J. S. Bell and R. Jackiw, A PCAC puzzle: π0→γγ in the σ model, Nuovo Cimento 60A, 47 (1969).
  35. F. R. Klinkhamer and N. S. Manton, A saddle point solution in the Weinberg-Salam theory, Phys. Rev. D 30, 2212 (1984).
  36. S. H. H. Tye and S. S. C. Wong, Bloch wave function for the periodic sphaleron potential and unsuppressed baryon and lepton number violating processes, Phys. Rev. D 92, 045005 (2015).
  37. S. H. H. Tye and S. S. C. Wong, The Chern–Simons number as a dynamical variable, Ann. Math. Sci. Appl. 1, 123 (2016).
  38. V. A. Rubakov, Superheavy magnetic monopoles and proton decay, JETP Lett. 33, 644 (1981).
  39. V. A. Rubakov, Adler-Bell-Jackiw anomaly and fermion number breaking in the presence of a magnetic monopole, Nucl. Phys. B203, 311 (1982).
  40. C. G. Callan, Jr., Monopole catalysis of baryon decay, Nucl. Phys. B212, 391 (1983).
  41. J. R. Ellis, D. V. Nanopoulos, and K. A. Olive, Baryon number violation catalyzed by grand unified monopoles, Phys. Lett. 116B, 127 (1982).
  42. D. Kharzeev, E. Shuryak, and I. Zahed, Sphalerons, baryogenesis, and helical magnetogenesis in the electroweak transition of the minimal Standard Model, Phys. Rev. D 102, 073003 (2020).
  43. S. S. AbdusSalam and T. A. Chowdhury, Scalar representations in the light of electroweak phase transition and cold dark matter phenomenology, J. Cosmol. Astropart. Phys. 05 (2014) 026.
  44. K. Hally, H. E. Logan, and T. Pilkington, Constraints on large scalar multiplets from perturbative unitarity, Phys. Rev. D 85, 095017 (2012).
  45. K. Earl, K. Hartling, H. E. Logan, and T. Pilkington, Constraining models with a large scalar multiplet, Phys. Rev. D 88, 015002 (2013).
  46. M. Cirelli, N. Fornengo, and A. Strumia, Minimal dark matter, Nucl. Phys. B753, 178 (2006).
  47. K. Kajantie, M. Laine, K. Rummukainen, and M. E. Shaposhnikov, Generic rules for high temperature dimensional reduction and their application to the standard model, Nucl. Phys. B458, 90 (1996).
  48. E. Braaten and A. Nieto, Effective field theory approach to high temperature thermodynamics, Phys. Rev. D 51, 6990 (1995).
  49. K. Farakos, K. Kajantie, K. Rummukainen, and M. E. Shaposhnikov, 3-D physics and the electroweak phase transition: Perturbation theory, Nucl. Phys. B425, 67 (1994).
  50. J. Löfgren, M. J. Ramsey-Musolf, P. Schicho, and T. V. I. Tenkanen, Nucleation at finite temperature: A gauge-invariant perturbative framework, Phys. Rev. Lett. 130, 251801 (2023).
  51. J. Hirvonen, J. Löfgren, M. J. Ramsey-Musolf, P. Schicho, and T. V. I. Tenkanen, Computing the gauge-invariant bubble nucleation rate in finite temperature effective field theory, J. High Energy Phys. 07 (2022) 135.
  52. W. J. G. de Blok, The core-cusp problem, Adv. Astron. 2010, 789293 (2010).
  53. S. Tulin and H.-B. Yu, Dark matter self-interactions and small scale structure, Phys. Rep. 730, 1 (2018).
  54. Q.-H. Cao, K. Hashino, X.-X. Li, and J.-H. Yue, Multistep phase transition and gravitational wave from general Z2 scalar extensions, Phys. Rev. D 111, 095003 (2025).
  55. M. Quiros, Finite temperature field theory and phase transitions, in ICTP Summer School in High-Energy Physics and Cosmology (1999), pp. 187–259 arXiv:hep-ph/9901312.
  56. S. Navas et al. (Particle Data Group), Review of particle physics, Phys. Rev. D 110, 030001 (2024).
  57. S. Inoue, G. Ovanesyan, and M. J. Ramsey-Musolf, Two-step electroweak baryogenesis, Phys. Rev. D 93, 015013 (2016).
  58. Z. Bo et al. (PandaX Collaboration), Dark matter search results from 1.54 Tonne year exposure of PandaX-4T, Phys. Rev. Lett. 134, 011805 (2025).
  59. J. Aalbers et al., Dark matter search results from 4.2 tonne-years of exposure of the LUX-ZEPLIN (LZ) experiment, Phys. Rev. Lett. 135, 011802 (2025).
  60. T. Akiba, H. Kikuchi, and T. Yanagida, Static minimum energy path from a vacuum to a sphaleron in the Weinberg-Salam model, Phys. Rev. D 38, 1937 (1988).
  61. K. T. Matchev and S. Verner, The electroweak sphaleron revisited: I. Static solutions, energy barrier, and unstable modes, arXiv:2505.05607.
  62. B. Kleihaus, J. Kunz, and Y. Brihaye, The electroweak sphaleron at physical mixing angle, Phys. Lett. B 273, 100 (1991).
  63. M. A. Luty, Baryogenesis via leptogenesis, Phys. Rev. D 45, 455 (1992).
  64. T. D. Brennan, L.-T. Wang, and H. Xiao, Monopole catalyzed baryogenesis with a θ angle, arXiv:2412.14239.

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