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| CMS-HIG-24-017 ; CERN-EP-2025-280 | ||
| Search for a boosted Higgs boson decaying to bottom quark pairs in association with a W or Z boson in proton-proton collisions at $ \sqrt{s} = $ 13 TeV | ||
| CMS Collaboration | ||
| 8 January 2026 | ||
| Submitted to Physics Letters B | ||
| Abstract: A search is conducted for standard model Higgs bosons with large transverse momentum ($ p_{\mathrm{T}} $) decaying to bottom quark pairs and produced in association with a hadronically decaying W or Z boson at the LHC. The result is based on a dataset of proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector in 2016--2018, corresponding to an integrated luminosity of 138 fb$ ^{-1} $. Boosted Higgs, W, and Z boson decays are reconstructed using large-radius jets with $ p_{\mathrm{T}} > $ 450 GeV and identified with heavy-flavor classifiers based on a graph convolutional neural network. The observed signal strength relative to the standard model expectation is $ \mu= $ 0.72 $ ^{+0.75}_{-0.71} $ including statistical and systematic uncertainties. | ||
| Links: e-print arXiv:2601.05362 [hep-ex] (PDF) ; CDS record ; inSPIRE record ; CADI line (restricted) ; | ||
| Figures | |
png pdf |
Figure 1:
The Higgs boson candidate $ m_\mathrm{SD} $ distribution in the $ \mathcal{D}(\mathrm{b}\overline{\mathrm{b}}\text{ vs. QCD}) $ fail (left) and pass region (right), both in the category with V candidate mass between 68 and 110 GeV. The grey bands in the lower panels represent the systematic uncertainty in the background prediction. The $ \mathrm{V}(\mathrm{q}\mathrm{q})\mathrm{Z}(\mathrm{b}\overline{\mathrm{b}}) $ process is separated from other $ \mathrm{V}(\mathrm{q}\mathrm{q})\mathrm{V}(\mathrm{q}\mathrm{q}) $ processes since it is used to validate the analysis strategy. |
png pdf |
Figure 1-a:
The Higgs boson candidate $ m_\mathrm{SD} $ distribution in the $ \mathcal{D}(\mathrm{b}\overline{\mathrm{b}}\text{ vs. QCD}) $ fail (left) and pass region (right), both in the category with V candidate mass between 68 and 110 GeV. The grey bands in the lower panels represent the systematic uncertainty in the background prediction. The $ \mathrm{V}(\mathrm{q}\mathrm{q})\mathrm{Z}(\mathrm{b}\overline{\mathrm{b}}) $ process is separated from other $ \mathrm{V}(\mathrm{q}\mathrm{q})\mathrm{V}(\mathrm{q}\mathrm{q}) $ processes since it is used to validate the analysis strategy. |
png pdf |
Figure 1-b:
The Higgs boson candidate $ m_\mathrm{SD} $ distribution in the $ \mathcal{D}(\mathrm{b}\overline{\mathrm{b}}\text{ vs. QCD}) $ fail (left) and pass region (right), both in the category with V candidate mass between 68 and 110 GeV. The grey bands in the lower panels represent the systematic uncertainty in the background prediction. The $ \mathrm{V}(\mathrm{q}\mathrm{q})\mathrm{Z}(\mathrm{b}\overline{\mathrm{b}}) $ process is separated from other $ \mathrm{V}(\mathrm{q}\mathrm{q})\mathrm{V}(\mathrm{q}\mathrm{q}) $ processes since it is used to validate the analysis strategy. |
png pdf |
Figure 2:
The Higgs boson candidate $ m_\mathrm{SD} $ distribution in the $ \mathcal{D}(\mathrm{b}\overline{\mathrm{b}}\text{ vs. QCD}) $ fail (left) and pass region (right) regions, in the category where the V candidate $ m_\mathrm{SD} $ is in the range 40--68 GeV (upper) and 110--201 GeV (lower). Other details are as described in the caption of Fig. 1. |
png pdf |
Figure 2-a:
The Higgs boson candidate $ m_\mathrm{SD} $ distribution in the $ \mathcal{D}(\mathrm{b}\overline{\mathrm{b}}\text{ vs. QCD}) $ fail (left) and pass region (right) regions, in the category where the V candidate $ m_\mathrm{SD} $ is in the range 40--68 GeV (upper) and 110--201 GeV (lower). Other details are as described in the caption of Fig. 1. |
png pdf |
Figure 2-b:
The Higgs boson candidate $ m_\mathrm{SD} $ distribution in the $ \mathcal{D}(\mathrm{b}\overline{\mathrm{b}}\text{ vs. QCD}) $ fail (left) and pass region (right) regions, in the category where the V candidate $ m_\mathrm{SD} $ is in the range 40--68 GeV (upper) and 110--201 GeV (lower). Other details are as described in the caption of Fig. 1. |
png pdf |
Figure 2-c:
The Higgs boson candidate $ m_\mathrm{SD} $ distribution in the $ \mathcal{D}(\mathrm{b}\overline{\mathrm{b}}\text{ vs. QCD}) $ fail (left) and pass region (right) regions, in the category where the V candidate $ m_\mathrm{SD} $ is in the range 40--68 GeV (upper) and 110--201 GeV (lower). Other details are as described in the caption of Fig. 1. |
png pdf |
Figure 2-d:
The Higgs boson candidate $ m_\mathrm{SD} $ distribution in the $ \mathcal{D}(\mathrm{b}\overline{\mathrm{b}}\text{ vs. QCD}) $ fail (left) and pass region (right) regions, in the category where the V candidate $ m_\mathrm{SD} $ is in the range 40--68 GeV (upper) and 110--201 GeV (lower). Other details are as described in the caption of Fig. 1. |
| Tables | |
png pdf |
Table 1:
Fitted signal strengths and their total uncertainties for the VH and VZ processes, shown individually for each data-taking period and for the combined dataset. |
| Summary |
| A search for standard model Higgs boson (H) candidates with high transverse momentum ($ p_{\mathrm{T}} $) decaying to bottom quark pairs ($ \mathrm{b}\overline{\mathrm{b}} $) in association with a hadronically decaying W or Z (V) boson at the LHC has been presented. The analysis identifies collision events containing boosted hadronic jets with $ p_{\mathrm{T}} > $ 450 GeV and with substructure and flavor properties characteristic of $ \mathrm{H}\to\mathrm{b}\overline{\mathrm{b}} $ and hadronic V decays. The signal strength for the $ \mathrm{V}(\mathrm{q}\mathrm{q})\mathrm{H}(\mathrm{b}\overline{\mathrm{b}}) $ process extracted from a maximum likelihood fit to the data in the large-radius jet mass distribution is $ \mu_{\mathrm{V}\mathrm{H}}= $ 0.72 $ ^{+0.75}_{-0.71} $ including statistical and systematic uncertainties. This corresponds to a significance of 1.00 standard deviations ($ \sigma $), compared to 1.64 $ \sigma $ expected. The sensitivity of this measurement is primarily limited by the amount of data available. |
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