- Letter
- Open Access
First-order electroweak phase transition with a gauge-invariant approach
Phys. Rev. D 111, L051702 – Published 31 March, 2025
DOI: https://doi.org/10.1103/PhysRevD.111.L051702
Abstract
We study the electroweak phase transition with a three-dimensional standard model effective field theory at the two-loop level under a gauge-invariant approach. We observe that the phase transition parameters obtained with the gauge-invariant approach deviate from that obtained in the Landau gauge at around the percent level. We give the strongly first-order phase transition condition for electroweak baryogenesis and find that the predicted gravitational wave signals would be reduced for the new physics scale , and the parameter spaces of can be probed by the space-based interferometers, such as LISA, TianQin, and Taiji.
Physics Subject Headings (PhySH)
Article Text
Supplemental Material
References (57)
- D. E. Morrissey and M. J. Ramsey-Musolf, New J. Phys. 14, 125003 (2012).
- J. Yang and L. Bian, Phys. Rev. D 106, 023510 (2022).
- Y. Di, J. Wang, R. Zhou, L. Bian, R.-G. Cai, and J. Liu, Phys. Rev. Lett. 126, 251102 (2021).
- Y. Zhang, T. Vachaspati, and F. Ferrer, Phys. Rev. D 100, 083006 (2019).
- T. Stevens, M. B. Johnson, L. S. Kisslinger, and E. M. Henley, Phys. Rev. D 85, 063003 (2012).
- T. Kahniashvili, A. G. Tevzadze, and B. Ratra, Astrophys. J. 726, 78 (2011).
- M. Hindmarsh and A. Everett, Phys. Rev. D 58, 103505 (1998).
- D. Grasso and A. Riotto, Phys. Lett. B 418, 258 (1998).
- J. Ahonen and K. Enqvist, Phys. Rev. D 57, 664 (1998).
- R. Roshan and G. White, Rev. Mod. Phys. 97, 015001 (2025).
- P. Athron, C. Balázs, A. Fowlie, L. Morris, and L. Wu, Prog. Part. Nucl. Phys. 135, 104094 (2024).
- C. Caprini et al., J. Cosmol. Astropart. Phys. 04 (2016) 001.
- M. D’Onofrio, K. Rummukainen, and A. Tranberg, Phys. Rev. Lett. 113, 141602 (2014).
- Y. Hu, Phys. Rev. D 54, 1614 (1996).
- H. H. Patel and M. J. Ramsey-Musolf, J. High Energy Phys. 07 (2011) 029.
- N. K. Nielsen, Nucl. Phys. B101, 173 (1975).
- M. Garny and T. Konstandin, J. High Energy Phys. 07 (2012) 189.
- J. Hirvonen, J. Löfgren, M. J. Ramsey-Musolf, P. Schicho, and T. V. I. Tenkanen, J. High Energy Phys. 07 (2022) 135.
- J. Löfgren, M. J. Ramsey-Musolf, P. Schicho, and T. V. I. Tenkanen, Phys. Rev. Lett. 130, 251801 (2023).
- P. Schicho, T. V. I. Tenkanen, and G. White, J. High Energy Phys. 11 (2022) 047.
- L. Niemi, M. J. Ramsey-Musolf, T. V. I. Tenkanen, and D. J. Weir, Phys. Rev. Lett. 126, 171802 (2021).
- D. Croon, O. Gould, P. Schicho, T. V. I. Tenkanen, and G. White, J. High Energy Phys. 04 (2021) 055.
- P. Athron, C. Balazs, A. Fowlie, L. Morris, G. White, and Y. Zhang, J. High Energy Phys. 01 (2023) 050.
- W. Buchmuller, Z. Fodor, and A. Hebecker, Phys. Lett. B 331, 131 (1994).
- A. Hebecker, The electroweak phase transition, Other thesis, 1995, arXiv:hep-ph/9506418.
- W. Buchmuller, Z. Fodor, and A. Hebecker, Nucl. Phys. B447, 317 (1995).
- K. Farakos, K. Kajantie, K. Rummukainen, and M. E. Shaposhnikov, Nucl. Phys. B425, 67 (1994).
- K. Farakos, K. Kajantie, K. Rummukainen, and M. E. Shaposhnikov, Nucl. Phys. B442, 317 (1995).
- K. Kajantie, M. Laine, K. Rummukainen, and M. E. Shaposhnikov, Nucl. Phys. B458, 90 (1996).
- A. Gynther, Phys. Rev. D 68, 016001 (2003).
- M. Laine, Phys. Rev. D 51, 4525 (1995).
It has been established that the 3D thermal SMEFT at two-loop level will reduce the renormalization scale dependence fairly well [22, 23]. For the research with 4d SMEFT, see [33, 34, 35, 36, 37, 38, 39, 40].
- R.-G. Cai, M. Sasaki, and S.-J. Wang, J. High Energy Phys. 08 (2017) 004.
- C. Grojean, G. Servant, and J. D. Wells, Phys. Rev. D 71, 036001 (2005).
- C. Delaunay, C. Grojean, and J. D. Wells, J. High Energy Phys. 04 (2008) 029.
- M. Chala, C. Krause, and G. Nardini, J. High Energy Phys. 07 (2018) 062.
- D. Bodeker, L. Fromme, S. J. Huber, and M. Seniuch, J. High Energy Phys. 02 (2005) 026.
- K. Hashino and D. Ueda, Phys. Rev. D 107, 095022 (2023).
- P. H. Damgaard, A. Haarr, D. O’Connell, and A. Tranberg, J. High Energy Phys. 02 (2016) 107.
- M. Postma and G. White, J. High Energy Phys. 03 (2021) 280.
- R. Qin and L. Bian, J. High Energy Phys. 08 (2024) 157.
- See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevD.111.L051702 for a figure that shows the limitation of the DR with high-temperature expansion at the range .
- A. Ekstedt, O. Gould, and J. Hirvonen, J. High Energy Phys. 12 (2023) 056.
- M. Hindmarsh, S. J. Huber, K. Rummukainen, and D. J. Weir, Phys. Rev. D 96, 103520 (2017); 101, 089902(E) (2020).
- J. R. Espinosa, T. Konstandin, J. M. No, and G. Servant, J. Cosmol. Astropart. Phys. 06 (2010) 028.
- A. D. Sakharov, Pis’ma Zh. Eksp. Teor. Fiz. 5, 32 (1967).
- V. A. Kuzmin, V. A. Rubakov, and M. E. Shaposhnikov, Phys. Lett. 155B, 36 (1985).
- M. E. Shaposhnikov, Nucl. Phys. B287, 757 (1987).
- R. Zhou, L. Bian, and H.-K. Guo, Phys. Rev. D 101, 091903 (2020).
- X. Gan, A. J. Long, and L.-T. Wang, Phys. Rev. D 96, 115018 (2017).
- C. Caprini, R. Durrer, and G. Servant, Phys. Rev. D 77, 124015 (2008).
- S. J. Huber and T. Konstandin, J. Cosmol. Astropart. Phys. 09 (2008) 022.
- M. Hindmarsh, S. J. Huber, K. Rummukainen, and D. J. Weir, Phys. Rev. Lett. 112, 041301 (2014).
- M. Hindmarsh, S. J. Huber, K. Rummukainen, and D. J. Weir, Phys. Rev. D 92, 123009 (2015).
- C. Caprini, R. Durrer, and G. Servant, J. Cosmol. Astropart. Phys. 12 (2009) 024.
- G. D. Moore and K. Rummukainen, Phys. Rev. D 63, 045002 (2001).
- G. D. Moore, K. Rummukainen, and A. Tranberg, J. High Energy Phys. 04 (2001) 017.