CMS-TOP-18-014 ; CERN-EP-2021-222 | ||
Combination of inclusive top-quark pair production cross-section measurements using ATLAS and CMS data at √s= 7 and 8 TeV | ||
ATLAS and CMS Collaborations | ||
25 May 2022 | ||
JHEP 07 (2023) 213 | ||
Abstract: A combination of measurements of the inclusive top-quark pair production cross-section performed by ATLAS and CMS in proton-proton collisions at centre-of-mass energies of 7 and 8 TeV at the LHC is presented. The cross-sections are obtained using top-quark pair decays with an opposite-charge electron-muon pair in the final state and with data corresponding to an integrated luminosity of about 5 fb−1 at √s= 7 TeV and about 20 fb−1 at √s= 8 TeV for each experiment. The combined cross-sections are determined to be 178.5 ± 4.7 pb at √s= 7 TeV and 243.3+6.0−5.9 pb at √s= 8 TeV with a correlation of 0.41, using a reference top-quark mass value of 172.5 GeV. The ratio of the combined cross-sections is determined to be R8/7= 1.363 ± 0.032. The combined measured cross-sections and their ratio agree well with theory calculations using several parton distribution function (PDF) sets. The values of the top-quark pole mass (with the strong coupling fixed at 0.118) and the strong coupling (with the top-quark pole mass fixed at 172.5 GeV) are extracted from the combined results by fitting a next-to-next-to-leading-order plus next-to-next-to-leading-log QCD prediction to the measurements. Using a version of the NNPDF3.1 PDF set containing no top-quark measurements, the results obtained are mpolet= 173.4+1.8−2.0 GeV and αs(mZ)= 0.1170+0.0021−0.0018. | ||
Links: e-print arXiv:2205.13830 [hep-ex] (PDF) ; CDS record ; inSPIRE record ; HepData record ; CADI line (restricted) ; |
Figures | |
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Figure 1:
Measured tˉt production cross-sections at √s= 7 and 8 TeV compared with predictions using different PDF sets. NNPDF3.1_a is a version of this PDF set containing no top-quark measurements. The shaded bands represent the total uncertainties in the predictions. |
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Figure 2:
Measured ratios of the tˉt production cross-sections at √s= 7 and 8 TeV compared with predictions using different PDF sets. NNPDF3.1_a is a version of this PDF set containing no top-quark measurements. The shaded bands represent the total uncertainties in the predictions. |
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Figure 3:
Dependence of the predicted cross-section and the combined measured cross-section on (left) the top-quark pole mass mpolet and (right) the strong coupling αS(mZ). The prediction is evaluated for three different PDF sets and assumes (left) αS(mZ)= 0.118 ± 0.001 or (right) mpolet= 172.5 ± 1.0 GeV. NNPDF3.1_a is a version of this PDF set containing no top-quark measurements. The uncertainty bands include the effects of the uncertainties in the combined cross-sections and of the factorisation and renormalisation scale and PDF uncertainties in the predicted cross-sections. |
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Figure 3-a:
Dependence of the predicted cross-section and the combined measured cross-section on the top-quark pole mass mpolet. The prediction is evaluated for three different PDF sets and assumes αS(mZ)= 0.118 ± 0.001. NNPDF3.1_a is a version of this PDF set containing no top-quark measurements. The uncertainty bands include the effects of the uncertainties in the combined cross-sections and of the factorisation and renormalisation scale and PDF uncertainties in the predicted cross-sections. |
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Figure 3-b:
Dependence of the predicted cross-section and the combined measured cross-section on the strong coupling αS(mZ). The prediction is evaluated for three different PDF sets and assumes mpolet= 172.5 ± 1.0 GeV. NNPDF3.1_a is a version of this PDF set containing no top-quark measurements. The uncertainty bands include the effects of the uncertainties in the combined cross-sections and of the factorisation and renormalisation scale and PDF uncertainties in the predicted cross-sections. |
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Figure 4:
Dependence of the top-quark pole mass, mpolet, on the assumed value for the strong coupling, αS(mZ), including constraints from the combined measured cross-sections for three different PDF sets. NNPDF3.1_a is a version of this PDF set containing no top-quark measurements. The shaded band represents the 68% CL uncertainty on the extracted αS(mZ) when fixing mpolet and on mpolet when fixing αS(mZ). The uncertainty bands include the effects of the uncertainties in the combined cross-sections and of the renormalisation and factorisation scale and PDF uncertainties in the predicted cross-sections. |
Tables | |
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Table 1:
Predicted tˉt production cross-sections at different centre-of-mass energies and for different PDF sets. The uncertainties comprise PDF and αS uncertainties as well as uncertainties in the renormalisation and factorisation scales. The ratio of the predicted tˉt production cross-sections at √s= 8 TeV and 7 TeV, R8/7, is also shown. NNPDF3.1_a is a version of this PDF set containing no top-quark measurements. |
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Table 2:
Summary of the relative statistical, systematic and total uncertainties in the ATLAS measurements of the tˉt production cross-section, σtˉt, at √s= 7 and 8 TeV from Ref. [15], where ID stands for identification and JES for jet-energy scale, and the grouping is modified to allow for the combination with the CMS measurements. |
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Table 3:
Illustrative summary of the individual contributions to the total uncertainty in the CMS tˉt cross-section measurements from Ref. [19], where ID stands for identification, JES for jet-energy scale, ME for matrix element and PS for parton shower. |
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Table 4:
Assumed correlations between ATLAS and CMS systematic uncertainties. The assigned sign is based on the nature of the systematic uncertainty (e.g., minus for an `up' variation in the ATLAS measurement that corresponds to a `down' variation in the CMS measurement due to conventions within the collaborations). If the sign is ambiguous, the sign maximising the total uncertainty in the combined cross-section is chosen. Any uncertainties not included in the table are considered uncorrelated. |
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Table 5:
Illustration of the impact Δσtˉt/σtˉt of the dominant groups of systematic uncertainties on the combined cross-sections at √s= 7 and 8 TeV. |
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Table 6:
Measured mpolet and αS(mZ) values for each PDF set using the measured 7 and 8 TeV combined cross-sections. NNPDF3.1_a is a version of this PDF set containing no top-quark measurements. |
Summary |
A combination of measurements of the inclusive tˉt production cross-section performed by the ATLAS and CMS experiments at √s= 7 and 8 TeV is presented, accounting for correlations between the measurements from different experiments as well as correlations within the ATLAS and CMS measurements. The resulting cross-sections are σtˉt(√s=8 TeV)=243.3+6.0−5.9pb. The combined results improve on the precision of the most precise individual results by 25% at √s= 7 TeV, and by 28% at √s= 8 TeV, making these combined results the most precise measurements of the inclusive tˉt cross-section to date at those respective centre-of-mass energies. The correlation between the combined cross-sections values is 0.41, and their ratio is determined to be Furthermore, the combined values for σtˉt are used to determine the top-quark pole mass and the strong coupling by comparing them with the predicted evolution of σtˉt as a function of mpolet and αS(mZ), for different PDF sets. The measurement yields the most precise values, mpolet= 173.4+1.8−2.0 GeV (1.2% relative uncertainty) and αS(mZ)= 0.1170+0.0021−0:0018 (1.8% relative uncertainty), when using the NNPDF3.1_a PDF set. The extracted αS(mZ) value is more precise than previous measurements performed using top-quark event. |
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Compact Muon Solenoid LHC, CERN |
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