Search for a new resonance decaying to a Higgs boson and a scalar boson in events with two b jets and two Z bosons in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV

The CMS collaboration
CMS-B2G-24-022, 2026.

Abstract (data abstract)
A search is performed for a new resonance X decaying into either a pair of Higgs bosons (HH) or into a Higgs boson and a new scalar boson Y (HY), using proton-proton collision data collected at $\sqrt{s}=13 \text{TeV}$, corresponding to an integrated luminosity of 138$\,\text{fb}^{-1}$. This study performs a comprehensive exploitation of the bbZZ events, encompassing the following decay topologies. One H candidate is identified through its decay into a bottom quark-antiquark pair, while the other H or the Y candidate is selected through its decay into a pair of Z bosons. One Z boson is required to decay leptonically and the other, to decay into a pair of quarks or neutrinos. Events of interest are categorized based on the Lorentz boosts of the hadronically decaying H and Z bosons. Machine-learning-based discriminants, together with the reconstructed resonance mass, are employed across the different categories to separate signal from backgrounds, and their corresponding distributions are included in a simultaneous fit. No significant deviations from the standard model predictions are observed. Upper limits at the 95% confidence level are set on the HH and HY production cross sections. For resonant HH production, the upper limit on the cross section of $\mathrm{pp}\to \mathrm{X}\to \mathrm{HH}$ production is 1 pb for a high-mass resonance. For HY production, the upper limit on the cross section of the process $\mathrm{pp}\to \mathrm{X}\to \mathrm{HY} \to \mathrm{bbZZ}$ is approximately 5 fb for a high-mass resonance. This is comparable to the sensitivity achieved in other analyses, which focus on H decays to $\gamma\gamma$ or $\tau\tau$ and Y decays into a pair of bottom quarks or massive vector bosons.

  • Figure 2a

    Data from Figure 2 (upper left), located on page 11.

    10.17182/hepdata.167417.v1/t1

    Pre-fit distributions of $\Delta R(\ell,\ell)$ in the SR qq0M, combining the electron and muon channel and using all three data-taking...

  • Figure 2b

    Data from Figure 2 (upper right), located on page 11.

    10.17182/hepdata.167417.v1/t2

    Pre-fit distributions of HT in the SR qq0M, combining the electron and muon channel and using all three data-taking years....

  • Figure 2c

    Data from Figure 2 (lower left), located on page 11.

    10.17182/hepdata.167417.v1/t3

    Pre-fit distributions of $\Delta R(\ell_1,b_1)$ in the SR qq0M, combining the electron and muon channel and using all three data-taking...

  • Figure 2d

    Data from Figure 2 (lower right), located on page 11.

    10.17182/hepdata.167417.v1/t4

    Pre-fit distributions of $\Delta R(\ell_1,b_2)$ in the SR qq0M, combining the electron and muon channel and using all three data-taking...

  • Figure 3a

    Data from Figure 3 (upper left), located on page 13.

    10.17182/hepdata.167417.v1/t5

    The BDT score $\mathrm{S_{BDT}}$ distribution in the fully resolved SR qq0M. The backgrounds distributions are from post-fit; three pre-fit distributions...

  • Figure 3b

    Data from Figure 3 (upper right), located on page 13.

    10.17182/hepdata.167417.v1/t6

    The resonance mass $\mathrm{m^{rec}_{X}}$ distribution in the semi-boosted SR qqZM. The backgrounds distributions are from post-fit; three pre-fit distributions of...

  • Figure 3c

    Data from Figure 3 (lower left), located on page 13.

    10.17182/hepdata.167417.v1/t7

    The resonance mass $\mathrm{m^{rec}_{X}}$ distribution in the semi-boosted SR qqHM. The backgrounds distributions are from post-fit; three pre-fit distributions of...

  • Figure 3d

    Data from Figure 3 (lower right), located on page 13.

    10.17182/hepdata.167417.v1/t8

    The resonance mass $\mathrm{m^{rec}_{X}}$ distribution in the fully-boosted SR qq2M. The backgrounds distributions are from post-fit; three pre-fit distributions of...

  • Figure 4a

    Data from Figure 4 (left), located on page 14.

    10.17182/hepdata.167417.v1/t9

    The BDT score $\mathrm{S_{BDT}}$ distribution in the fully resolved SR $\nu\nu$0M. The backgrounds distributions are from post-fit; three pre-fit distributions...

  • Figure 4b

    Data from Figure 4 (right), located on page 14.

    10.17182/hepdata.167417.v1/t10

    The transverse resonance mass $\mathrm{m^{rec}_{X\prime}}$ distribution in the boosted SR $\nu\nu$1M. The backgrounds distributions are from post-fit; three pre-fit distributions...

  • Figure 5

    Data from Figure 5, located on page 16.

    10.17182/hepdata.167417.v1/t11

    Exclusion limits on the product of the production of HH through a resonance X.

  • Figure 6a

    Data from Figure 6 (left), located on page 17.

    10.17182/hepdata.167417.v1/t12

    Two-dimensional exclusion limits on the product of the production of $\mathrm{pp}\rightarrow \mathrm{X} \rightarrow \mathrm{HY} \rightarrow \mathrm{bbZZ}$.

  • Figure 6b

    Data from Figure 6 (right), located on page 17.

    10.17182/hepdata.167417.v1/t13

    Two-dimensional exclusion limits on the product of the production of $\mathrm{pp}\rightarrow \mathrm{X} \rightarrow \mathrm{HY} \rightarrow \mathrm{bbZZ}$.

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