CMS-HIG-14-016 ; CERN-PH-EP-2015-195 | ||
Measurement of differential cross sections for Higgs boson production in the diphoton decay channel in pp collisions at √s= 8 TeV | ||
CMS Collaboration | ||
29 August 2015 | ||
Eur. Phys. J. C 76 (2016) 13 | ||
Abstract: A measurement is presented of differential cross sections for the Higgs boson (H) production in pp collisions at √s= 8 TeV. The analysis exploits the H→γγ decay in data corresponding to an integrated luminosity of 19.7 fb−1 collected by the CMS experiment at the LHC. The cross section is measured as a function of the kinematic properties of the diphoton system and of the associated jets. Results corrected for detector effects are compared with predictions at next-to-leading order and next-to-next-to-leading order in perturbative quantum chromodynamics, as well as with predictions beyond the standard model.For isolated photons with pseudorapidities |η|< 2.5, and with the photon of largest and next-to-largest transverse momentum (pγT) divided by the diphoton mass mγγ satisfying the respective conditions of pγT/mγγ> 1/3 and > 1/4, the total fiducial cross section is 32 ± 10 fb. | ||
Links: e-print arXiv:1508.07819 [hep-ex] (PDF) ; CDS record ; inSPIRE record ; HepData record ; CADI line (restricted) ; |
Figures | |
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Figure 1-a:
Photon identification efficiencies for a Higgs boson with mH= 125 GeV , as a function of photon pseudorapidity (a), and photon transverse momentum (b). |
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Figure 1-b:
Photon identification efficiencies for a Higgs boson with mH= 125 GeV , as a function of photon pseudorapidity (a), and photon transverse momentum (b). |
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Figure 2-a:
Mass resolution estimator σm/mγγ after the decorrelation procedure, in Z→e+e− events in data (dots) and simulated events (histogram) with their systematic uncertainties (shaded bands) for barrel-barrel events (a), all the other events (b). The ratio of data to MC predictions are shown below each panel, and the error bars on each point represent the statistical uncertainties of the data. |
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Figure 2-b:
Mass resolution estimator σm/mγγ after the decorrelation procedure, in Z→e+e− events in data (dots) and simulated events (histogram) with their systematic uncertainties (shaded bands) for barrel-barrel events (a), all the other events (b). The ratio of data to MC predictions are shown below each panel, and the error bars on each point represent the statistical uncertainties of the data. |
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Figure 3:
Sum of the signal+background (S+B) model fits to the events of the three σm/mγγ classes in the fiducial phase space measurement, weighted by S/(S+B) separately in each category, together with the data binned as a function of mγγ. The 1 and 2 standard deviation bands of uncertainty (labeled as 1σ and 2σ) shown for the background component include the uncertainty due to the choice of function and the uncertainty in the fitted parameters. The bottom panel shows the result after subtracting the background component. |
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Figure 4-a:
The H→γγ differential cross section for inclusive events as a function of (a) pγγT, (upper right) |yγγ|, (lower left) Δϕγγ, and (lower right) |cosθ∗|. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013). Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. The last bin of pγγT distribution sums the events above 200 GeV . For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 4-b:
The H→γγ differential cross section for inclusive events as a function of (a) pγγT, (upper right) |yγγ|, (lower left) Δϕγγ, and (lower right) |cosθ∗|. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013). Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. The last bin of pγγT distribution sums the events above 200 GeV . For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 4-c:
The H→γγ differential cross section for inclusive events as a function of (a) pγγT, (upper right) |yγγ|, (lower left) Δϕγγ, and (lower right) |cosθ∗|. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013). Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. The last bin of pγγT distribution sums the events above 200 GeV . For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 4-d:
The H→γγ differential cross section for inclusive events as a function of (a) pγγT, (upper right) |yγγ|, (lower left) Δϕγγ, and (lower right) |cosθ∗|. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013). Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. The last bin of pγγT distribution sums the events above 200 GeV . For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 5-a:
The H→γγ differential cross section for H+jets events as a function of (a) pTj1, (b) |yγγ−yj1|, (c) Njets, with jets within |η|<2.5, and (d) mjj with jets within |η|<4.7. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013). Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. In each distribution, the last bin corresponds to the sum over the events beyond the bins shown in the figure. For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 5-b:
The H→γγ differential cross section for H+jets events as a function of (a) pTj1, (b) |yγγ−yj1|, (c) Njets, with jets within |η|<2.5, and (d) mjj with jets within |η|<4.7. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013). Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. In each distribution, the last bin corresponds to the sum over the events beyond the bins shown in the figure. For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 5-c:
The H→γγ differential cross section for H+jets events as a function of (a) pTj1, (b) |yγγ−yj1|, (c) Njets, with jets within |η|<2.5, and (d) mjj with jets within |η|<4.7. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013). Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. In each distribution, the last bin corresponds to the sum over the events beyond the bins shown in the figure. For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 5-d:
The H→γγ differential cross section for H+jets events as a function of (a) pTj1, (b) |yγγ−yj1|, (c) Njets, with jets within |η|<2.5, and (d) mjj with jets within |η|<4.7. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013). Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. In each distribution, the last bin corresponds to the sum over the events beyond the bins shown in the figure. For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 6-a:
The H→γγ differential cross section for H+2 jets events, with jets within |η|<4.7, as a function of (a) Δϕjj, (b) Δηjj, (c) Zeppenfeld variable, and (d) Δϕγγ,jj. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013).. Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. In the Zeppenfeld distribution, the last bin sums the events with values above 1.2. For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 6-b:
The H→γγ differential cross section for H+2 jets events, with jets within |η|<4.7, as a function of (a) Δϕjj, (b) Δηjj, (c) Zeppenfeld variable, and (d) Δϕγγ,jj. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013).. Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. In the Zeppenfeld distribution, the last bin sums the events with values above 1.2. For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 6-c:
The H→γγ differential cross section for H+2 jets events, with jets within |η|<4.7, as a function of (a) Δϕjj, (b) Δηjj, (c) Zeppenfeld variable, and (d) Δϕγγ,jj. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013).. Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. In the Zeppenfeld distribution, the last bin sums the events with values above 1.2. For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
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Figure 6-d:
The H→γγ differential cross section for H+2 jets events, with jets within |η|<4.7, as a function of (a) Δϕjj, (b) Δηjj, (c) Zeppenfeld variable, and (d) Δϕγγ,jj. All the SM contributions are normalized to their cross section from the LHC Higgs Cross Section Working Group (2013).. Theoretical uncertainties in the renormalization and factorization scales, PDF, and branching fraction are added in quadrature. The error bars on data points reflect both statistical and systematic uncertainties. In the Zeppenfeld distribution, the last bin sums the events with values above 1.2. For each graph, the bottom panel shows the ratio of data to theoretical predictions from POWHEG generator. |
Tables | |
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Table 1:
Values of the pp→H→γγ differential cross sections as a function of kinematic observables as measured in data and as predicted in SM simulations. For each observable the fit to mγγ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit ˆmH varies from observable to observable. |
Summary |
A measurement was carried out of differential cross sections as a function of kinematic observables in the H→γγ decay channel, using data collected by the CMS experiment √s= 8 TeV, corresponding to an integrated luminosity of 19.7 fb−1. The measurement was performed for events with two isolated photons in the kinematic range pγ1T/mγγ> 1/3 and pγ2T/mγγ> 1/4, with photon pseudorapidities within |η|< 2.5. Photon identification was chosen to reduce the dependence of the measurement on the kinematics of the signal. Event classification relied on an estimator of diphoton mass resolution. The signal extraction and the unfolding of experimental resolution were performed simultaneously in all bins of the chosen observables. In this kinematic range, the fiducial cross section was measured to be 32 ± 10 fb. The differential cross section of the Higgs boson was measured, inclusively in the number of jets, as a function of its transverse momentum pγγT, its rapidity |yγγ|, the Collins-Soper angular variable cosθ∗, the difference in azimuthal angle between the two photons Δϕγγ, and the number of associated jets Njets. The transverse momentum of the leading jet pj1T, and the difference in rapidity between the Higgs boson and the leading jet |yγγ−yj1| were determined in events with at least one accompanying jet. In events with at least two jets, measurements were made of the dijet mass mjj, the azimuth between the two jets Δϕjj, the pseudorapidity difference between the two jets Δηjj, the Zeppenfeld variable |ηγγ−(ηj1+ηj2)/2|, and the azimuthal angle between the Higgs boson and the dijet system Δϕγγ,jj. The differential cross sections were compared with several SM and beyond SM calculations, and found to be compatible with the SM predictions within statistical, systematic, and theoretical uncertainties. |
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Compact Muon Solenoid LHC, CERN |
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