CMS-PAS-HIG-17-009 | ||
Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV | ||
CMS Collaboration | ||
November 2017 | ||
Abstract: A search for a narrow-width resonance decaying into two Higgs bosons, each having a mass of 125 GeV and decaying into a bˉb pair, is presented. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 35.9 fb−1 at √s= 13 TeV recorded by the CMS detector at the LHC. No evidence for a signal is observed and upper limits at a 95% confidence level on the production cross section times branching fraction for such a resonance decaying to two Higgs bosons and each of them to bˉb are set in the mass range from 260 to 1200 GeV. | ||
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These preliminary results are superseded in this paper, JHEP 08 (2018) 152. The superseded preliminary plots can be found here. |
Figures | |
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Figure 1:
The selection efficiency for simulated X→H(bˉb)H(bˉb) events (X is a spin-2 Bulk KK-Graviton) at different stages of the event selection for each mass hypothesis, for the low-mass region (solid) and the medium-mass region (dashed). The vertical line at 580 GeV shows corresponds to the transition between twe two selections. |
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Figure 2:
The mX distribution of signal simulated events (spin-2 Bulk KK-Graviton) after the event selection criteria for the 450, 750 and 1000 GeV mass hypotheses, with and without the correction by the kinematic constraint to mH and the specific b-jet energy corrections. |
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Figure 3:
Illustration of SR and SB in the (mH1, mH2) plane used to motivate and validate the parametric model for the QCD multijet background. The quantities mH1 and mH2 are the two reconstructed Higgs boson masses after b tagging and kinematic selections for data in medium-mass region. |
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Figure 4:
The mX predicted (blue) distribution in data for the low-mass signal region in the lower fit range and the actual distribution in the signal region (black). |
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Figure 5:
The mX distribution in the sideband (SB) of the medium-mass region is presented in data. |
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Figure 6:
The mX distributions after the LMR selections for prediction of the Signal Region. These distributions are fitted in the two sub-ranges with both nominal and alternative model ([250,330] GeV (left) [285,625] GeV (right)). A fit to the background-only hypothesis, which consists of the QCD multijet shape is shown. The shaded regions correspond to a ±1 and 2 σ variation of this parametrized form. |
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Figure 6-a:
The mX distributions after the LMR selections for prediction of the Signal Region. These distributions are fitted in the two sub-ranges with both nominal and alternative model ([250,330] GeV). A fit to the background-only hypothesis, which consists of the QCD multijet shape is shown. The shaded regions correspond to a ±1 and 2 σ variation of this parametrized form. |
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Figure 6-b:
The mX distributions after the LMR selections for prediction of the Signal Region. These distributions are fitted in the two sub-ranges with both nominal and alternative model ([285,625] GeV). A fit to the background-only hypothesis, which consists of the QCD multijet shape is shown. The shaded regions correspond to a ±1 and 2 σ variation of this parametrized form. |
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Figure 7:
The mX distribution of the QCD multijet component of the background in the Signal Region in data for the MMR. A fit to the background-only hypothesis, which consists of the QCD multijet shape is shown. The shaded regions correspond to a ±1 and 2 σ variation of this parametrized form. |
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Figure 8:
The observed and expected upper limits on the cross section for a spin-2 resonance X→H(bˉb)H(bˉb) at a 95% confidence level using data corresponding to an integrated luminosity of 35.9 fb−1 at √s= 13 TeV using the asymptotic CLS method. Theoretical cross section for the Bulk KK-Graviton, with k/MPl= 0.5, kl= 35, decaying to four b jets via Higgs bosons is overlaid. The transition between LMR and MMR is based on the expected sensitivity, resulting in the observed discontinuity. |
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Figure 9:
The observed and expected upper limits on the cross section for a spin-0 resonance X→H(bˉb)H(bˉb) at a 95% confidence level using data corresponding to an integrated luminosity of 35.9 fb−1 at √s= 13 TeV using the asymptotic CLS method. Theoretical cross section for the radion, with λbda= 3 TeV, kl= 35, and no radion-Higgs boson mixing, decaying to four b jets via Higgs bosons is overlaid. The transition between LMR and MMR is based on the expected sensitivity, resulting in the observed discontinuity. |
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Figure 10:
Observed and expected 95% confidence level upper limits on the production cross section times branching fraction for a spin-2 resonance decaying to HH, using data corresponding to an integrated luminosity of 35.9 fb−1 at √s= 13 TeV. The results from different searches investigating various combinations of Higgs boson decay modes are reported. |
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Figure 11:
Observed and expected 95% confidence level upper limits on the production cross section times branching fraction for a spin-0 resonance decaying to HH, using data corresponding to an integrated luminosity of 35.9 fb−1 at √s= 13 TeV. The results from different searches investigating various combinations of Higgs boson decay modes are reported. |
Tables | |
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Table 1:
Definitions of the regions we use in the "ABCD" method to test the functional form as described in text. |
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Table 2:
Impact of systematic uncertainties on the signal efficiencies in the low-mass region (LMR) and the medium-mass region (MMR). |
Summary |
A search for a narrow-width resonance decaying into two Higgs bosons, each having a mass of 125 GeV and decaying into a bˉb pair, is presented. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 35.9 fb−1 at √s= 13 TeV recorded by the CMS detector at the LHC. No evidence for a signal is observed and upper limits at a 95% confidence level on the production cross section for such spin-0 and spin-2 resonances, in the mass range from 260 to 1200 GeV, are set. Using these results, a radion with decay constant of 3 TeV and a bulk graviton with k set to 0.5MPl are excluded at a 95% confidence level in the mass range from 300 to 1100 GeV and 320 to 720 GeV respectively. |
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Compact Muon Solenoid LHC, CERN |
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