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  • Open Access

Higgs couplings in SMEFT via Zh production at the HL-LHC

Subhaditya Bhattacharya1,*, Sanjoy Biswas2,†, and Abhik Sarkar1,‡

  • *Contact author: subhab@iitg.ac.in
  • †Contact author: sanjoy.phy@gm.rkmvu.ac.in
  • ‡Contact author: sarkar.abhik@iitg.ac.in

Phys. Rev. D 111, 115038 – Published 30 June, 2025

DOI: https://doi.org/10.1103/h3wk-gnfb

Abstract

We study the Higgs couplings involved in the Zh associated production mode at the Large Hadron Collider (LHC) in presence of Higgs-gauge boson coupling modifiers via κ framework and dimension-six Standard Model (SM) effective theory operators. The analysis is performed mainly in the context of the High-Luminosity LHC (with s=14  TeV and luminosity 3000  fb−1) setup using cut-based as well as machine learning techniques. The analysis shows significant betterment in the signal significance by using the machine learning technique. We also do a χ2 analysis, which reveals an appreciable change in the sensitivity of the coupling modifiers due to the presence of effective operators, in particular, due to the qqZh Higgs-current interactions. The dipole operators concerning the same vertex combine quarks of different chiralities and do not interfere with the SM diagrams, hence contributing only at O(Λ−4). In order to observe better sensitivity for this class of operators, we need to move to higher center-of-mass energy, where the effects of both Higgs-current and dipole four-point interactions are more prominent.

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Corrections

5 August, 2025

Correction: A grant number was missing in the Acknowledgments section and has been inserted.

Article Text

References (83)

  1. H. E. Logan, TASI 2013 Lectures on Higgs Physics within and Beyond the Standard Model (2014).
  2. Particle Data Group, Review of particle physics, Prog. Theor. Exp. Phys. 2022, 083C01 (2022).
  3. ATLAS Collaboration, A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery, Nature (London) 607, 52 (2022).
  4. CMS Collaboration, A portrait of the Higgs boson by the CMS experiment ten years after the discovery, Nature (London) 607, 60 (2022).
  5. CMS Collaboration, Constraints on anomalous HVV couplings from the production of Higgs bosons decaying to τ lepton pairs, Phys. Rev. D 100, 112002 (2019).
  6. I. Anderson et al., Constraining anomalous HVV interactions at proton and lepton Colliders, Phys. Rev. D 89, 035007 (2014).
  7. P. Sharma and A. Shivaji, Probing non-standard HVV(V=W,Z) couplings in single Higgs production at future electron-proton collider, J. High Energy Phys. 10 (2022) 108.
  8. A. I. Hernández-Juárez, G. Tavares-Velasco, and A. Fernández-Téllez, New evaluation of the HZZ coupling: Direct bounds on anomalous contributions and CP-violating effects via a new asymmetry, Phys. Rev. D 107, 115031 (2023).
  9. S. Dutta, K. Hagiwara, and Y. Matsumoto, Measuring the Higgs-Vector boson couplings at linear e+e− Collider, Phys. Rev. D 78, 115016 (2008).
  10. N. Desai, D. K. Ghosh, and B. Mukhopadhyaya, CP-violating HWW couplings at the large hadron collider, Phys. Rev. D 83, 113004 (2011).
  11. N. D. Christensen, T. Han, and Y. Li, Testing CP violation in ZZH interactions at the LHC, Phys. Lett. B 693, 28 (2010).
  12. S. Dwivedi, D. K. Ghosh, B. Mukhopadhyaya, and A. Shivaji, Distinguishing CP-odd couplings of the Higgs boson to weak boson pairs, Phys. Rev. D 93, 115039 (2016).
  13. F. U. Bernlochner, C. Englert, C. Hays, K. Lohwasser, H. Mildner, A. Pilkington, D. D. Price, and M. Spannowsky, Angles on CP-violation in Higgs boson interactions, Phys. Lett. B 790, 372 (2019).
  14. J. Brehmer, F. Kling, T. Plehn, and T. M. P. Tait, Better Higgs-CP tests through information geometry, Phys. Rev. D 97, 095017 (2018).
  15. S. Banerjee, T. Mandal, B. Mellado, and B. Mukhopadhyaya, Cornering dimension-6HVV interactions at high luminosity LHC: The role of event ratios, J. High Energy Phys. 09 (2015) 057.
  16. S. Banerjee, C. Englert, R. S. Gupta, and M. Spannowsky, Probing electroweak precision physics via boosted Higgs-strahlung at the LHC, Phys. Rev. D 98, 095012 (2018).
  17. S. Banerjee, R. S. Gupta, J. Y. Reiness, and M. Spannowsky, Resolving the tensor structure of the Higgs coupling to Z-bosons via Higgs-strahlung, Phys. Rev. D 100, 115004 (2019).
  18. S. Banerjee, R. S. Gupta, J. Y. Reiness, S. Seth, and M. Spannowsky, Towards the ultimate differential SMEFT analysis, J. High Energy Phys. 09 (2020) 170.
  19. F. F. Freitas, C. K. Khosa, and V. Sanz, Exploring the standard model EFT in VH production with machine learning, Phys. Rev. D 100, 035040 (2019).
  20. F. Bishara, P. Englert, C. Grojean, G. Panico, and A. N. Rossia, Revisiting Vh(→bb¯) at the LHC and FCC-hh, J. High Energy Phys. 06 (2023) 077.
  21. F. Bishara, S. De Curtis, L. Delle Rose, P. Englert, C. Grojean, M. Montull, G. Panico, and A. N. Rossia, Precision from the diphoton Zh channel at FCC-hh, J. High Energy Phys. 04 (2021) 154.
  22. P. Englert, Improved precision in Vh(→bb¯) via boosted decision trees, arXiv:2407.21239.
  23. S. Banerjee, R. S. Gupta, O. Ochoa-Valeriano, M. Spannowsky, and E. Venturini, A fully differential SMEFT analysis of the golden channel using the method of moments, J. High Energy Phys. 06 (2021) 031.
  24. S. Banerjee, R. S. Gupta, O. Ochoa-Valeriano, and M. Spannowsky, High energy lepton colliders as the ultimate Higgs microscopes, J. High Energy Phys. 02 (2022) 176.
  25. T. Biswas, A. Datta, and B. Mukhopadhyaya, Following the trail of new physics via the vector boson fusion Higgs boson signal at the large hadron collider, Phys. Rev. D 105, 055028 (2022).
  26. J. Y. Araz, S. Banerjee, R. S. Gupta, and M. Spannowsky, Precision SMEFT bounds from the VBF Higgs at high transverse momentum, J. High Energy Phys. 04 (2021) 125.
  27. H. T. Li, B. Yan, and C. P. Yuan, Discriminating between Higgs production mechanisms via jet charge at the LHC, Phys. Rev. Lett. 131, 041802 (2023).
  28. B. Yan, Determining Higgs boson width at electron-positron colliders, Phys. Lett. B 822, 136709 (2021).
  29. K.-P. Xie and B. Yan, Probing the electroweak symmetry breaking with Higgs production at the LHC, Phys. Lett. B 820, 136515 (2021).
  30. I. Brivio and M. Trott, The standard model as an effective field theory, Phys. Rep. 793, 1 (2019).
  31. Q. Bonnefoy, J. Kley, D. Liu, A. N. Rossia, and C.-Y. Yao, Aligned yet large dipoles: A SMEFT study, J. High Energy Phys. 11 (2024) 046.
  32. R. Alonso, E. E. Jenkins, and A. V. Manohar, A geometric formulation of Higgs effective field theory: Measuring the curvature of scalar field space, Phys. Lett. B 754, 335 (2016).
  33. A. Crivellin, M. Ghezzi, and M. Procura, Effective field theory with two Higgs doublets, J. High Energy Phys. 09 (2016) 160.
  34. Anisha, S. Das Bakshi, J. Chakrabortty, and S. Prakash, Hilbert series and plethystics: Paving the path towards 2HDM- and MLRSM-EFT, J. High Energy Phys. 09 (2019) 035.
  35. F. del Aguila, S. Bar-Shalom, A. Soni, and J. Wudka, Heavy Majorana neutrinos in the effective Lagrangian description: Application to hadron colliders, Phys. Lett. B 670, 399 (2009).
  36. A. Aparici, K. Kim, A. Santamaria, and J. Wudka, Right-handed neutrino magnetic moments, Phys. Rev. D 80, 013010 (2009).
  37. S. Bhattacharya and J. Wudka, Dimension-seven operators in the standard model with right handed neutrinos, Phys. Rev. D 94, 055022 (2016).
  38. Y. Liao and X.-D. Ma, Operators up to dimension seven in standard model effective field theory extended with sterile neutrinos, Phys. Rev. D 96, 015012 (2017).
  39. H.-L. Li, Z. Ren, J. Shu, M.-L. Xiao, J.-H. Yu, and Y.-H. Zheng, Complete set of dimension-eight operators in the standard model effective field theory, Phys. Rev. D 104, 015026 (2021).
  40. C. W. Murphy, Dimension-8 operators in the standard model effective field theory, J. High Energy Phys. 10 (2020) 174.
  41. B. Grzadkowski, M. Iskrzynski, M. Misiak, and J. Rosiek, Dimension-six terms in the standard model Lagrangian, J. High Energy Phys. 10 (2010) 085.
  42. S. Bhattacharya and J. Wudka, Effective theories with dark matter applications, Int. J. Mod. Phys. D 30, 2130004 (2021).
  43. A. Alloul, N. D. Christensen, C. Degrande, C. Duhr, and B. Fuks, feynrules 2.0—A complete toolbox for tree-level phenomenology, Comput. Phys. Commun. 185, 2250 (2014).
  44. C. Degrande, C. Duhr, B. Fuks, D. Grellscheid, O. Mattelaer, and T. Reiter, UFO—The universal feynrules output, Comput. Phys. Commun. 183, 1201 (2012).
  45. I. Brivio, smeftsim 3.0—A practical guide, J. High Energy Phys. 04 (2021) 073.
  46. C. Degrande, G. Durieux, F. Maltoni, K. Mimasu, E. Vryonidou, and C. Zhang, Automated one-loop computations in the standard model effective field theory, Phys. Rev. D 103, 096024 (2021).
  47. J. Alwall, M. Herquet, F. Maltoni, O. Mattelaer, and T. Stelzer, madgraph 5: Going beyond, J. High Energy Phys. 06 (2011) 128.
  48. CMS Collaboration, Observation of Higgs boson decay to bottom quarks, Phys. Rev. Lett. 121, 121801 (2018).
  49. ATLAS Collaboration, Measurements of WH and ZH production in the H→bb¯ decay channel in pp collisions at 13 TeV with the ATLAS detector, Eur. Phys. J. C 81, 178 (2021).
  50. R. Boughezal, E. Mereghetti, and F. Petriello, Dilepton production in the SMEFT at O(1/Λ4), Phys. Rev. D 104, 095022 (2021).
  51. E. da Silva Almeida, N. Rosa-Agostinho, O. J. P. Éboli, and M. C. Gonzalez-Garcia, Light-quark dipole operators at the LHC, Phys. Rev. D 100, 013003 (2019).
  52. SMEFiT Collaboration, Combined SMEFT interpretation of Higgs, diboson, and top quark data from the LHC, J. High Energy Phys. 11 (2021) 089.
  53. C. Grunwald, G. Hiller, K. Kröninger, and L. Nollen, More synergies from beauty, top, Z and Drell-Yan measurements in SMEFT, J. High Energy Phys. 11 (2023) 110.
  54. A. Buckley, C. Englert, J. Ferrando, D. J. Miller, L. Moore, M. Russell et al., Constraining top quark effective theory in the LHC run II era, J. High Energy Phys. 04 (2016) 015.
  55. J. Ellis, M. Madigan, K. Mimasu, V. Sanz, and T. You, Top, Higgs, Diboson and electroweak fit to the standard model effective field theory, J. High Energy Phys. 04 (2021) 279.
  56. I. Brivio, S. Bruggisser, N. Elmer, E. Geoffray, M. Luchmann, and T. Plehn, To profile or to marginalize—A SMEFT case study, SciPost Phys. 16, 035 (2024).
  57. Anisha, S. Das Bakshi, S. Banerjee, A. Biekötter, J. Chakrabortty, S. Kumar Patra, and M. Spannowsky, Effective limits on single scalar extensions in the light of recent LHC data, Phys. Rev. D 107, 055028 (2023).
  58. S. Bißmann, C. Grunwald, G. Hiller, and K. Kröninger, Top and beauty synergies in SMEFT-fits at present and future colliders, J. High Energy Phys. 06 (2021) 010.
  59. M. Thomas Arun, K. Deka, and T. Srivastava, Constraining SMEFT BSM scenarios with EWPO and ΔCKM, arXiv:2301.09273.
  60. ATLAS Collaboration, Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector, J. High Energy Phys. 07 (2021) 005.
  61. ATLAS Collaboration, Combined measurements of Higgs boson production and decay using up to 139  fb−1 of proton-proton collision data at s=13  TeV collected with the ATLAS experiment, Phys. Rev. D 101, 012002 (2020).
  62. ATLAS Collaboration, Combined effective field theory interpretation of Higgs boson and weak boson production and decay with ATLAS data and electroweak precision observables, CERN Report No. ATL-PHYS-PUB-2022-037, 2022, https://cds.cern.ch/record/2816369.
  63. J. de Blas, Y. Du, C. Grojean, J. Gu, V. Miralles, M. E. Peskin et al., Global SMEFT fits at future colliders, in Snowmass 2021 (2022).
  64. E. Celada, T. Giani, J. ter Hoeve, L. Mantani, J. Rojo, A. N. Rossia, M. O. A. Thomas, and E. Vryonidou, Mapping the SMEFT at high-energy colliders: From LEP and the (HL-)LHC to the FCC-ee, J. High Energy Phys. 09 (2024) 091.
  65. C. Bissolotti, R. Boughezal, and K. Simsek, SMEFT probes in future precision DIS experiments, Phys. Rev. D 108, 075007 (2023).
  66. V. Cirigliano, A. Crivellin, W. Dekens, J. de Vries, M. Hoferichter, and E. Mereghetti, CP violation in Higgs-gauge interactions: From tabletop experiments to the LHC, Phys. Rev. Lett. 123, 051801 (2019).
  67. J. Kley, T. Theil, E. Venturini, and A. Weiler, Electric dipole moments at one-loop in the dimension-6 SMEFT, Eur. Phys. J. C 82, 926 (2022).
  68. G. Panico, A. Pomarol, and M. Riembau, EFT approach to the electron electric dipole moment at the two-loop level, J. High Energy Phys. 04 (2019) 090.
  69. R. D. Ball et al., Parton distributions with LHC data, Nucl. Phys. B867, 244 (2013).
  70. T. Sjostrand, S. Mrenna, and P. Z. Skands, A brief introduction to pythia 8.1, Comput. Phys. Commun. 178, 852 (2008).
  71. M. Cacciari, G. P. Salam, and G. Soyez, FastJet user manual, Eur. Phys. J. C 72, 1896 (2012).
  72. M. Cacciari, G. P. Salam, and G. Soyez, The anti-kt jet clustering algorithm, J. High Energy Phys. 04 (2008) 063.
  73. E. Conte, B. Fuks, and G. Serret, madanalysis 5, A user-friendly framework for collider phenomenology, Comput. Phys. Commun. 184, 222 (2013).
  74. F. Cascioli, T. Gehrmann, M. Grazzini, S. Kallweit, P. Maierhöfer, A. von Manteuffel, S. Pozzorini, D. Rathlev, L. Tancredi, and E. Weihs, ZZ production at hadron colliders in NNLO QCD, Phys. Lett. B 735, 311 (2014).
  75. L. Chen, J. Davies, G. Heinrich, S. P. Jones, M. Kerner, G. Mishima, J. Schlenk, and M. Steinhauser, ZH production in gluon fusion at NLO in QCD, J. High Energy Phys. 08 (2022) 056.
  76. J. M. Campbell, J. W. Huston, and W. J. Stirling, Hard interactions of quarks and gluons: A primer for LHC physics, Rep. Prog. Phys. 70, 89 (2007).
  77. M. D. Schwartz, TASI lectures on collider physics, in Proceedings, Theoretical Advanced Study Institute in Elementary Particle Physics: Anticipating the Next Discoveries in Particle Physics (TASI 2016): Boulder, CO, USA, June 6-July 1, 2016, edited by R. Essig and I. Low (, Singapore, 2018), pp. 65–100, 10.1142/9789813233348_0002.
  78. G. Cowan, K. Cranmer, E. Gross, and O. Vitells, Asymptotic formulae for likelihood-based tests of new physics, Eur. Phys. J. C 71, 1554 (2011).
  79. Y. Coadou, Boosted decision trees, Artificial Intelligence for High Energy Physics (World Scientific, Singapore, 2022), pp. 9–58.
  80. A. S. Cornell, W. Doorsamy, B. Fuks, G. Harmsen, and L. Mason, Boosted decision trees in the era of new physics: A smuon analysis case study, J. High Energy Phys. 04 (2022) 015.
  81. T. Chen and C. Guestrin, Xgboost: A scalable tree boosting system, in Proceedings of the 22nd ACM SIGKDD International Conference on Knowledge Discovery and Data Mining, KDD ’16, ACM (2016).
  82. F. Pedregosa, G. Varoquaux, A. Gramfort, V. Michel, B. Thirion, O. Grisel et al., scikit-learn: Machine learning in python, J. Mach. Learn. Res. 12, 2825 (2011), http://jmlr.org/papers/v12/pedregosa11a.html.
  83. S. Lundberg and S.-I. Lee, A unified approach to interpreting model predictions, arXiv:1705.07874.

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