CMS-HIG-20-004 ; CERN-EP-2022-114 | ||
Search for nonresonant Higgs boson pair production in the four leptons plus two b jets final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV | ||
CMS Collaboration | ||
22 June 2022 | ||
JHEP 06 (2023) 130 | ||
Abstract: The first search for nonresonant production of Higgs boson pairs (HH) with one H decaying into four leptons and the other into a pair of b quarks is presented, using proton-proton collisions recorded at a center-of-mass energy of $\sqrt{s} = $ 13 TeV by the CMS experiment. The analyzed data correspond to an integrated luminosity of 138 fb$^{-1}$. A 95% confidence level upper limit of 32.4 is set on the signal strength modifier $\mu$, defined as the ratio of the observed HH production rate in the ${\mathrm{H}\mathrm{H}} \to\mathrm{Z}\mathrm{Z}^{*}\mathrm{b}\mathrm{\bar{b}}\to 4\ell\mathrm{b}\mathrm{\bar{b}}$ decay channel to the standard model expectation. Possible modifications of the H trilinear coupling $\lambda_\text{HHH}$ with respect to the standard model (SM) value are investigated. The coupling modifier $\kappa_{\lambda}$, defined as $\lambda_\text{HHH}$ divided by its SM prediction, is constrained to be within the observed (expected) range $-$8.8 ($-$9.8) $ < \kappa_{\lambda} < $ 13.4 (15.0) at 95% confidence level. | ||
Links: e-print arXiv:2206.10657 [hep-ex] (PDF) ; CDS record ; inSPIRE record ; HepData record ; CADI line (restricted) ; |
Figures | |
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Figure 1:
Feynman diagrams contributing to Higgs boson pair production via gluon-gluon fusion in the SM at LO. |
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Figure 2:
The $m(4\ell)$ (left) and $m(\mathrm{b} \mathrm{\bar{b}})$ (right) distributions. The $m(\mathrm{b} \mathrm{\bar{b}})$ plot is drawn after the selection: 115 $ < m(4\ell) < $ 135 GeV. In the ratio plot, the grey dashed shades represent the relative statistical uncertainty on the total estimated background. |
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Figure 2-a:
The $m(4\ell)$ (left) and $m(\mathrm{b} \mathrm{\bar{b}})$ (right) distributions. The $m(\mathrm{b} \mathrm{\bar{b}})$ plot is drawn after the selection: 115 $ < m(4\ell) < $ 135 GeV. In the ratio plot, the grey dashed shades represent the relative statistical uncertainty on the total estimated background. |
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Figure 2-b:
The $m(4\ell)$ (left) and $m(\mathrm{b} \mathrm{\bar{b}})$ (right) distributions. The $m(\mathrm{b} \mathrm{\bar{b}})$ plot is drawn after the selection: 115 $ < m(4\ell) < $ 135 GeV. In the ratio plot, the grey dashed shades represent the relative statistical uncertainty on the total estimated background. |
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Figure 3:
Inclusive BDT distributions for simulated signal, estimated background components, and data for the combination of the three different final states (4$\mu $, 4e, and 2e2$\mu $) and data-taking years. In the ratio plot, the grey dashed shades represent the relative statistical uncertainty on the total estimated background. |
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Figure 4:
Left: upper limit on the signal strength at 95% CL for each year and for their combination. Right: expected and observed 95% CL upper limits on the SM-like HH production cross section obtained for different values of $\kappa _\lambda $. The green and yellow bands represent, respectively, the one and two standard deviation (s.d.) quantiles around the expected limit. The red curve is the HH theoretical prediction cross section as a function of $\kappa _\lambda $. |
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Figure 4-a:
Left: upper limit on the signal strength at 95% CL for each year and for their combination. Right: expected and observed 95% CL upper limits on the SM-like HH production cross section obtained for different values of $\kappa _\lambda $. The green and yellow bands represent, respectively, the one and two standard deviation (s.d.) quantiles around the expected limit. The red curve is the HH theoretical prediction cross section as a function of $\kappa _\lambda $. |
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Figure 4-b:
Left: upper limit on the signal strength at 95% CL for each year and for their combination. Right: expected and observed 95% CL upper limits on the SM-like HH production cross section obtained for different values of $\kappa _\lambda $. The green and yellow bands represent, respectively, the one and two standard deviation (s.d.) quantiles around the expected limit. The red curve is the HH theoretical prediction cross section as a function of $\kappa _\lambda $. |
Tables | |
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Table 1:
Expected yields in the 4$\ell $ SR after additionally requiring at least two jets in the event. "Others'' represents contributions from $\mathrm{t} \mathrm{\bar{t}} $W, WWZ, WZZ, and ZZZ processes. |
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Table 2:
Summary of experimental systematic uncertainties. The effect of b-tagging SF, JER, and JES is propagated to the shape of the BDT distribution. |
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Table 3:
Summary of the theory systematic uncertainties considered in this analysis. |
Summary |
The first search for nonresonant Higgs boson (H) pair production in the four lepton $\mathrm{b}\mathrm{\bar{b}}$ final state is presented. This search uses a data sample collected in proton-proton collisions at $\sqrt{s} = =$ 13 TeV by the CMS detector during the years 2016-2018 corresponding to an integrated luminosity of 138 fb$^{-1}$. The results are found to be compatible with the standard model (SM) expectations. An observed (expected) upper limit on the HH production cross section is set at 32.4 (39.6) times the SM expected rate at the 95% confidence level. Possible modifications of the H trilinear coupling $\lambda_\text{HHH}$ with respect to the standard model (SM) value are investigated. The coupling modifier $\kappa_{\lambda}$, defined as $\lambda_\text{HHH}$ divided by its SM prediction, is constrained to be within the observed (expected) range $-$8.8 ($-$9.8) $ < \kappa_{\lambda} < $ 13.4 (15.0) at 95% confidence level. The limits set by this analysis are complementary with those obtained by more sensitive channels, despite the lower branching fraction of the $4\ell\mathrm{b}\mathrm{\bar{b}}$ final state. |
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