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Measurement of the ttbar production cross section using dilepton events in ppbar collisions
High Energy Physics - Experiment · Submitted 26 May 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This result combined with the cross section measurement in the lepton + jets final state yields sigma(ttbar)=7.56 +0.63-0.56 (stat + syst) pb, which agrees with the standard model expectation.
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The abstract, sentence by sentence
We present a measurement of the ttbar production cross section sigma(ttbar) in ppbar collisions at sqrt{s} = 1.96 TeV using 5.4 fb-1 of integrated luminosity collected with the D0 detector. We consider final states with at least two jets and two leptons (ee, emu, mumu), and events with one jet for the the emu final state as well. The measured cross section is sigma(ttbar)= 7.36 +0.90-0.79 (stat + syst) pb. This result combined with the cross section measurement in the lepton + jets final state yields sigma(ttbar)=7.56 +0.63-0.56 (stat + syst) pb, which agrees with the standard model expectation. The relative precision of 8% of this measurement is comparable to the latest theoretical calculations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a measurement of the ttbar production cross section sigma(ttbar) in ppbar collisions at sqrt{s} = 1.96 TeV using 5.4 fb-1 of integrated luminosity collected with the D0 detector. | contribution 0.96 | 0.96 | 0.08 | asserted 1.00 |
| s1 | We consider final states with at least two jets and two leptons (ee, emu, mumu), and events with one jet for the the emu final state as well. | method 0.95 | 0.68 | 0.02 | asserted 0.86 |
| s2 | The measured cross section is sigma(ttbar)= 7.36 +0.90-0.79 (stat + syst) pb. | result 1.00 | 0.98 | 0.59 | asserted 1.00 |
| s3 | This result combined with the cross section measurement in the lepton + jets final state yields sigma(ttbar)=7.56 +0.63-0.56 (stat + syst) pb, which agrees with the standard model expectation. | result 0.92 | 0.92 | 0.62 | asserted 0.88 |
| s4 | The relative precision of 8% of this measurement is comparable to the latest theoretical calculations. | interpretation 0.96 | 0.68 | 0.11 | asserted 1.00 |
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The paper
Original abstract
We present a measurement of the ttbar production cross section sigma(ttbar) in ppbar collisions at sqrt{s} = 1.96 TeV using 5.4 fb-1 of integrated luminosity collected with the D0 detector. We consider final states with at least two jets and two leptons (ee, emu, mumu), and events with one jet for the the emu final state as well. The measured cross section is sigma(ttbar)= 7.36 +0.90-0.79 (stat + syst) pb. This result combined with the cross section measurement in the lepton + jets final state yields sigma(ttbar)=7.56 +0.63-0.56 (stat + syst) pb, which agrees with the standard model expectation. The relative precision of 8% of this measurement is comparable to the latest theoretical calculations.
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References
How the literature uses it
19 arXiv papers cite this in 34 sentences
Papers citing it · 13 sentences without a confident label
Uses its method or tool 1 paper
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For the channel, we use the same selections as used for the measurement of the cross section described in Ref. [ref] .
Precision measurement of the ratio B(t -> Wb)/B(t -> Wq) · Introduction · 0.98
Uses its data or values 11 papers
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Since LHC data of top-pair productions have been updated, however, we also re-derive new limits on $d_V$ and $d_A$ combining the recent data from the Tevatron for $√(s)=1.96$ TeV and the LHC for $√(s)=7$ TeV assuming $m_t=172.5$ GeV: σ_exp = 7.50±0.48 [pb], (CDF [ref] ) = 7.56^+0.63_-0.56 [pb], (D0 [ref] ) = 187^+22_-21 [pb], (ATLAS [ref] ) = 165.8 ±13.3 [pb].
Optimal-observable Analysis of Possible Non-standard Top-quark Couplings in pp -> t t-bar X -> l^+ X' · section.subsection.$$#1 · 1.00
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The two vertical lines in the figure corresponds to the 1-$σ$ boundaries of the maximum allowed $σ_tt̅$ at the Tevatron [ref] .
Top quark physics in the Vector Color-Octet Model · $tt̅$ production and distribution · 0.92
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We thus use the following Tevatron data and the corresponding SM estimates: * Inclusive $t t̅$ cross section from D0 [ref] and the QCD NNLO calculation [ref] . * Differential $t t̅$ cross section as a function of $$ from CDF [ref] (Table 3, all bins but the first), to be compared with the approximate NNLO calculation of [ref] (Fig. 12). * Inclusive $t t̅$ forward-backward asymmetry as measured by D0 in the lepton+jet channel [ref] and by CDF in the dilepton channel [ref] , and the corresponding NLO QCD+EW estimate quoted by CDF in [ref] . * Differential $t t̅$ forward-backward asymmetry as a function of $$ from CDF and the NLO QCD+EW estimate [ref] (Table XVII).
Predictions from Heavy New Physics Interpretation of the Top Forward-Backward Asymmetry · Global Fit to the Top Tevatron Data · 0.99
Compares with it 4 papers
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At the Tevatron the total top-pair cross section is $7.08 ^+0.00_-0.24 ^+0.36_-0.27$ pb [ref] , in very good agreement with recent results from CDF [ref] and D0 [ref] .
NNLL threshold resummation for top-pair and single-top production · Introduction · 0.85
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This is investigated in Figure [ref], where the NNLL prediction for the total cross section obtained with the MSTW2008 [ref] , CT10 [ref] , NNPDF2.1 [ref] and ABM11 [ref] NNLO PDF sets are compared to each other and to the measurements provided by [ref] .
The total top-pair production cross section at NNLL · The $t t̅$ total cross section at NNLL · 0.90
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The results are in agreement with each other, and the extracted cross sections are consistent with those from Refs. [ref] .
Precision measurement of the ratio B(t -> Wb)/B(t -> Wq) · Introduction · 1.00
Cites it as background 1 paper
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In addition to the production cross section for $$ and single top events in $pp$ [ref] and $pp̅$ [ref] collisions, various properties of the top quark have been studied.
Measurement of the inclusive ttgamma cross section at sqrt(s) = 7 TeV with the ATLAS detector · Top quark properties and experimental results · 0.98
What it cites · 1 sentence without a confident label
Uses the method or tool of 1 paper
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Jets are identified with a cone algorithm with radius $R<0.5$ [ref] in the range $|η|< 2.5$.
Run II Jet Physics: Proceedings of the Run II QCD and Weak Boson Physics Workshop · Object Identification · 1.00
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