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PreprintCC BY 4.0arXiv

Using Higgs Boson Production in Association with Three Jets via Gluon Fusion at the LHC to Investigate the CP Properties of the Higgs Boson

Abstract

A neutral Higgs boson Φ with general scalar and pseudoscalar couplings and accompanying jets can be efficiently produced via gluon fusion through heavy-quark loops in high-energy hadronic collisions. We present integrated cross sections and kinematic distributions for the production of a generic Higgs boson Φ in association with three jets, pp → Φjjj, at order αs5. We include the full mass dependence of the top- and bottom-quark loop contributions, combined coherently so that their interference is retained. Earlier finite-mass calculations of Φ+3 jets with bottom-quark loops and CP-odd or CP-mixed couplings were restricted to gg → gggΦ; we include the complete set of partonic subprocesses, and find that the quark-containing channels supply close to one half of the pseudoscalar three-jet cross section at tanβ=1. In a Type-II two-Higgs-doublet model the bottom-quark loop comes to dominate the rate as tanβ is increased, so that the cross section is non-monotonic in tanβ. Comparing against the heavy-top effective theory and its form-factor-improved version, we show that the effective description fails in the hard tails of the transverse-momentum and dijet-mass distributions, while the third-jet centrality z⋆ and the rapidity separation of the two leading jets are largely insensitive to the heavy-quark treatment. We further study the multi-jet azimuthal correlation Φ2, built from the jet momenta on the two sides of the Higgs boson in rapidity, and find that the bottom-quark contribution modifies its shape even for a state of definite CP. For a CP-mixed state the interference of the two couplings adds a sin2Φ2 term, which a simple counting asymmetry isolates and which no CP eigenstate can produce. Numerical results are presented for the LHC at √s=13.6TeV and mΦ=125.2GeV.

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BibTeX
@misc{bhattacharya2026using,
  title = {{Using Higgs Boson Production in Association with Three Jets via Gluon Fusion at the LHC to Investigate the CP Properties of the Higgs Boson}},
  author = {Arunima Bhattacharya and Francisco Campanario and Michael Kubocz and Terrance Figy and Tunde Kushimo and Ivan Rosario},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.37627},
  eprint = {2610.37627},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.37627},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Using Higgs Boson Production in Association with Three Jets via Gluon Fusion at the LHC to Investigate the CP Properties of the Higgs Boson
AU  - Arunima Bhattacharya
AU  - Francisco Campanario
AU  - Michael Kubocz
AU  - Terrance Figy
AU  - Tunde Kushimo
AU  - Ivan Rosario
PY  - 2026
DA  - 2026/10/27
PB  - arXiv
DO  - 10.48550/arxiv.2610.37627
UR  - https://arxiv.org/abs/2610.37627
AB  - A neutral Higgs boson Φ with general scalar and pseudoscalar couplings and accompanying jets can be efficiently produced via gluon fusion through heavy-quark loops in high-energy hadronic collisions. We present integrated cross sections and kinematic distributions for the production of a generic Higgs boson Φ in association with three jets, pp → Φjjj, at order α_s^5. We include the full mass dependence of the top- and bottom-quark loop contributions, combined coherently so that their interference is retained. Earlier finite-mass calculations of Φ+3 jets with bottom-quark loops and CP-odd or CP-mixed couplings were restricted to gg → gggΦ; we include the complete set of partonic subprocesses, and find that the quark-containing channels supply close to one half of the pseudoscalar three-jet cross section at tanβ=1. In a Type-II two-Higgs-doublet model the bottom-quark loop comes to dominate the rate as tanβ is increased, so that the cross section is non-monotonic in tanβ. Comparing against the heavy-top effective theory and its form-factor-improved version, we show that the effective description fails in the hard tails of the transverse-momentum and dijet-mass distributions, while the third-jet centrality z^⋆ and the rapidity separation of the two leading jets are largely insensitive to the heavy-quark treatment. We further study the multi-jet azimuthal correlation Φ_2, built from the jet momenta on the two sides of the Higgs boson in rapidity, and find that the bottom-quark contribution modifies its shape even for a state of definite CP. For a CP-mixed state the interference of the two couplings adds a sin2Φ_2 term, which a simple counting asymmetry isolates and which no CP eigenstate can produce. Numerical results are presented for the LHC at √s=13.6TeV and m_Φ=125.2GeV.
ER  -