- Open Access
Probing neutral triple gauge couplings via production at colliders with machine learning
Phys. Rev. D 113, 075005 – Published 3 April, 2026
DOI: https://doi.org/10.1103/w9wn-fxkc
Abstract
Neutral triple gauge couplings (nTGCs) first arise from the dimension-8 operators of the Standard Model effective field theory (SMEFT), rather than the dimension-4 SM Lagrangian and dimension-6 SMEFT operators, opening up a unique window for probing new physics at the dimension-8 level. In this work, we formulate the nTGC form factors of (, ) that are compatible with the spontaneous breaking of the electroweak gauge symmetry and consistently match the dimension-8 nTGC operators in the broken phase. We study the sensitivities for probing both the form factors and the corresponding new physics scales through production (with visible/invisible fermionic decays) at high energy colliders including CEPC, FCC-ee, LCF, ILC, and CLIC. In particular, we identify the dimension-8 operator that contributes to the pure triple boson coupling alone, but not the mixed coupling. We further study the correlations between probes of the and couplings. Using machine learning, we show that angular distributions of the final-state fermions can play key roles in suppressing the SM backgrounds. The sensitivities can be further improved by using polarized beams, and we find that the optimal sensitivity bounds on the nTGC correlations are given by the mixed setting including both the unpolarized operation and the follow-up polarized operation. We demonstrate that machine learning is advantageous for handling the 4-body final states from decays and improves significantly the sensitivity reaches of probes of nTGCs in collisions. We find that nTGC new physics scales can be probed up to the multi-TeV scale at the proposed colliders.
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References (36)
- For reviews John Ellis, in The Conference Proceedings of “Beyond Standard Model: From Theory to Experiment” (BSM-2021), Zewail City, Egypt, March 29-31, 2021 (2021); I. Brivio and M. Trott, Phys. Rep. 793, 1 (2019); and references therein.
- J. Ellis, H.-J. He, and R.-Q. Xiao, Sci. China Phys. Mech. Astron. 68, 121062 (2025).
- J. Ellis, H.-J. He, and R.-Q. Xiao, Phys. Rev. D 108, L111704 (2023).
- J. Ellis, H.-J. He, and R.-Q. Xiao, Phys. Rev. D 107, 035005 (2023).
- D. Liu, R.-Q. Xiao, S. Li, J. Ellis, H.-J. He, and R. Yuan, Front. Phys. 20, 015201 (2025).
- J. Ellis, H.-J. He, and R.-Q. Xiao, Sci. China Phys. Mech. Astron. 64, 221062 (2021).
- J. Ellis, S. F. Ge, H.-J. He, and R.-Q. Xiao, Chin. Phys. C 44, 063106 (2020).
- J. Ellis, H.-J. He, R.-Q. Xiao, S.-P. Zeng, and J. Zheng, Phys. Rev. D 111, 015007 (2025).
- See also, R. Cepedello, F. Esser, M. Hirsch, and V. Sanz, J. High Energy Phys. 07 (2024) 275; 12 (2024) 84.
- G. J. Gounaris, J. Layssac, and F. M. Renard, Phys. Rev. D 61, 073013 (2000); 62, 073013 (2000).
- C. Degrande, J. High Energy Phys. 02 (2014) 101.
- V. Khachatryan et al. (CMS Collaboration), Phys. Lett. B 760, 448 (2016).
- M. Aaboud et al. (ATLAS Collaboration), J. High Energy Phys. 12 (2018) 010.
- ATLAS Collaboration, Measurements of differential cross sections and search for neutral triple gauge couplings in collisions at with the ATLAS detector, ATLAS-CONF-2025-001, 2025.
- W. Buchmuller and D. Wyler, Nucl. Phys. B268, 621 (1986); B. Grzadkowski, M. Iskrzynski, M. Misiak, and J. Rosiek, J. High Energy Phys. 10 (2010) 085; and references therein.
- E.g. J. Ellis, V. Sanz, and T. You, J. High Energy Phys. 07 (2014) 036; 03 (2015) 157; H. J. He, J. Ren, and W. Yao, Phys. Rev. D 93, 015003 (2016); J. Ellis and T. You, J. High Energy Phys. 03 (2016) 089; S. F. Ge, H. J. He, and R. Q. Xiao, 10 (2016) 007; J. de Blas, M. Ciuchini, E. Franco, S. Mishima, M. Pierini, L. Reina, and L. Silvestrini, 12 (2016) 135; F. Ferreira, B. Fuks, V. Sanz, and D. Sengupta, Eur. Phys. J. C 77, 675 (2017); J. Ellis, P. Roloff, V. Sanz, and T. You, J. High Energy Phys. 05 (2017) 096; G. Durieux, C. Grojean, J. Gu, and K. Wang, 09 (2017) 014; T. Barklow, K. Fujii, S. Jung, R. Karl, J. List, T. Ogawa, M. E. Peskin, and J. Tian, Phys. Rev. D 97, 053003 (2018); C. W. Murphy, 97, 015007 (2018); J. Ellis, C. W. Murphy, V. Sanz, and T. You, J. High Energy Phys. 06 (2018) 146; G. N. Remmen and N. L. Rodd, 12 (2019) 032; A. Gutierrez-Rodriguez, M. Koksal, A. A. Billur, and M. A. Hernandez-Ruiz, J. Phys. G 47, 055005 (2020); M. Koksal, A. A. Billur, A. Gutierrez-Rodriguez, and M. A. Hernandez-Ruiz, Phys. Lett. B808, 135661 (2020); J. Ellis, M. Madigan, K. Mimasu, V. Sanz, and T. You, J. High Energy Phys. 04 (2021) 279; and references therein.
- E.g. S. Jahedi, J. High Energy Phys. 12 (2023) 031; S. Spor, E. Gurkanli, and M. Köksal, arXiv:2302.08245; S. Jahedi and J. Lahiri, J. High Energy Phys. 04 (2023) 085; S. Spor, Nucl. Phys. B991, 116198 (2023); A. Senol, S. Spor, E. Gurkanli, V. Cetinkaya, H. Denizli, and M. Köksal, Eur. Phys. J. Plus 137, 1354 (2022); Q. Fu, J. C. Yang, C. X. Yue, and Y. C. Guo, Nucl. Phys. B972, 115543 (2021); A. Biekötter, P. Gregg, F. Krauss, and M. Schönherr, Phys. Lett. B817, 136311 (2021); A. Senol, H. Denizli, A. Yilmaz, I. Turk Cakir, K. Y. Oyulmaz, O. Karadeniz, and O. Cakir, Nucl. Phys. B935, 365 (2018); R. Rahaman and R. K. Singh, B948, 114754 (2019); Eur. Phys. J. C 77, 521 (2017); 76, 539 (2016).
- Y.-C. Guo, C.-J. Pan, M.-Q. Ruan, and J.-C. Yang, Phys. Rev. D 112, 035033 (2025).
- M. Chala, A. Diaz-Carmona, and G. Guedes, J. High Energy Phys. 05 (2022) 138.
- C. W. Murphy, J. High Energy Phys. 10 (2020) 174.
- H. L. Li, Z. Ren, J. Shu, M. L. Xiao, J. H. Yu, and Y. H. Zheng, Phys. Rev. D 104, 015026 (2021).
- D. A. Dicus and H.-J. He, Phys. Rev. D 71, 093009 (2005); Phys. Rev. Lett. 94, 221802 (2005).
- M. Jacob and G. C. Wick, Ann. Phys. (N.Y.) 7, 404 (1959).
- For a comprehensive review, H. J. He, Y. P. Kuang, and C. P. Yuan, arXiv:hep-ph/9704276; See also, H. J. He and W. B. Kilgore, Phys. Rev. D 55, 1515 (1997); H. J. He, Y. P. Kuang, and C. P. Yuan, 51, 6463 (1995); 55, 3038 (1997); H. J. He, Y. P. Kuang, and X. Li, Phys. Lett. B 329, 278 (1994); Phys. Rev. D 49, 4842 (1994); Phys. Rev. Lett. 69, 2619 (1992); and references therein.
- F. Englert and R. Brout, Phys. Rev. Lett. 13, 321 (1964); P. W. Higgs, 13, 508 (1964); Phys. Lett. 12, 132 (1964); G. S. Guralnik, C. R. Hagen, and T. Kibble, Phys. Rev. Lett. 13, 585 (1964); T. Kibble, Phys. Rev. 155, 1554 (1967).
- J. Alwall, R. Frederix, S. Frixione, V. Hirschi, F. Maltoni, O. Mattelaer, H. S. Shao, T. Stelzer, P. Torrielli, and M. Zaro, J. High Energy Phys. 07 (2014) 079.
- J. B. Guimaraes da Costa et al. (CEPC Study Group), arXiv:1811.10545.
- S. P. Adhya et al. (CEPC Study Group), arXiv:2510.05260; W. Abdallah et al., Radiat. Detect. Technol. Methods 8, 1 (2024).
- M. Benedikt, F. Zimmermann et al., Eur. Phys. J. C 85, 1468 (2025).
- H. Abramowicz et al. (Linear Collider Collaboration), arXiv:2503.24049.
- E. Adli et al. (CLIC collaboration and CLICdp Collaboration), arXiv:2503.24168.
- J. de Blas et al. (CLIC Collaboration), CERN Yellow Rep. Monogr. 3, 1 (2018); (CLIC Collaboration)CERN-TH-2018-267 and CERN-2018-009-M, arXiv:1812.02093, 10.23731/CYRM-2018-003.
- K. Fujii et al. (LCC Physics Working Group), arXiv:1710.07621; arXiv:2007.03650; M. E. Peskin, ILC: Open Questions and New Ideas, talk at the Snowmass Energy Frontier Workshop on Open Questions and New Ideas, Fermilab, USA, July 20-22 (2020);
- A. F. Zarnecki (CLICdp Collaboration and ILD Concept Group), Proc. Sci., CORFU2019 (2020) 037 [arXiv:2004.14628].
- T. Plehn, A. Butter, B. Dillon, T. Heimel, C. Krause, and R. Winterhalder, arXiv:2211.01421.
- K. Fujii, C. Grojean, M. E. Peskin et al. (The Linear Collider Collaboration Physics Working Group), arXiv:1801.02840.