{"arxiv_id":"1105.5384","incoming":{"papers":19,"sentences":34,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":2,"quotes":[{"arxiv_id":"1106.5436","title":"Precision measurement of the ratio B(t -> Wb)/B(t -> Wq)","url":"/paper/1106.5436","section":"Introduction","sentence":"For the channel, we use the same selections as used for the measurement of the cross section described in Ref. [ref] .","intent_p":0.98,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":11,"sentences":14,"quotes":[{"arxiv_id":"1206.2413","title":"Optimal-observable Analysis of Possible Non-standard Top-quark Couplings in pp -> t t-bar X -> l^+ X'","url":"/paper/1206.2413","section":"section.subsection.$$#1","sentence":"Since LHC data of top-pair productions have been updated, however, we also re-derive new limits on $d_V$ and $d_A$ combining the recent data from the Tevatron for $√(s)=1.96$ TeV and the LHC for $√(s)=7$ TeV assuming $m_t=172.5$ GeV: σ_exp = 7.50±0.48 [pb], (CDF [ref] ) = 7.56^+0.63_-0.56 [pb], (D0 [ref] ) = 187^+22_-21 [pb], (ATLAS [ref] ) = 165.8 ±13.3 [pb].","intent_p":1.0,"contests_p":null},{"arxiv_id":"1209.3636","title":"Top quark physics in the Vector Color-Octet Model","url":"/paper/1209.3636","section":"$tt̅$ production and distribution","sentence":"The two vertical lines in the figure corresponds to the 1-$σ$ boundaries of the maximum allowed $σ_tt̅$ at the Tevatron [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1207.0740","title":"Predictions from Heavy New Physics Interpretation of the Top Forward-Backward Asymmetry","url":"/paper/1207.0740","section":"Global Fit to the Top Tevatron Data","sentence":"We thus use the following Tevatron data and the corresponding SM estimates: * Inclusive $t t̅$ cross section from D0 [ref] and the QCD NNLO calculation [ref] . * Differential $t t̅$ cross section as a function of $$ 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 $$ from CDF and the NLO QCD+EW estimate [ref] (Table XVII).","intent_p":0.99,"contests_p":null},{"arxiv_id":"1205.5005","title":"Diquark contributions to Top quark charge asymmetry at the Tevatron and LHC","url":"/paper/1205.5005","section":"Total $tt̅$ cross section and asymmetries at Tevatron and LHC","sentence":"The condition eq.([ref]) for the total cross section is rather loose, since the observed $tt̅$ production cross sections [ref] tend to be somewhat larger than the NLO+NLL QCD prediction of about $7.14$ pb for $m_t=172.5$ GeV [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1206.4484","title":"Top Quark Physics at the LHC: A Review of the First Two Years","url":"/paper/1206.4484","section":"Top Quark Pair Production Cross Section","sentence":"The $$ cross section was measured in $pp̅$ collisions at the Tevatron ($√(s) = 1.96$), most precisely as $σ_= 7.56 ^+0.63_-0.56 pb$ (D0 [ref] , precision 8%) and $σ_= 7.50 ±0.48 pb$ (CDF [ref] , precision 6.4%), in good agreement with the SM prediction.","intent_p":0.96,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1210.7813","title":"NNLL threshold resummation for top-pair and single-top production","url":"/paper/1210.7813","section":"Introduction","sentence":"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] .","intent_p":0.85,"contests_p":null},{"arxiv_id":"1208.5578","title":"The total top-pair production cross section at NNLL","url":"/paper/1208.5578","section":"The $t t̅$ total cross section at NNLL","sentence":"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] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1106.5436","title":"Precision measurement of the ratio B(t -> Wb)/B(t -> Wq)","url":"/paper/1106.5436","section":"Introduction","sentence":"The results are in agreement with each other, and the extracted cross sections are consistent with those from Refs. [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1111.5869","title":"Top-pair production at hadron colliders with next-to-next-to-leading logarithmic soft-gluon resummation","url":"/paper/1111.5869","section":"Phenomenology","sentence":"On the same figures we compare our theoretical predictions with the most accurate available experimental measurements from the Tevatron [ref] , [ref] and LHC [ref] , [ref] .","intent_p":0.9,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1206.5696","title":"Measurement of the inclusive ttgamma cross section at sqrt(s) = 7 TeV with the ATLAS detector","url":"/paper/1206.5696","section":"Top quark properties and experimental results","sentence":"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.","intent_p":0.98,"contests_p":null}]}],"unlabelled_sentences":13},"outgoing":{"papers":2,"sentences":2,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"hep-ex/0005012","title":"Run II Jet Physics: Proceedings of the Run II QCD and Weak Boson Physics Workshop","url":"/paper/hep-ex/0005012","section":"Object Identification","sentence":"Jets are identified with a cone algorithm with radius $R<0.5$ [ref] in the range $|η|< 2.5$.","intent_p":1.0,"contests_p":null}]}],"unlabelled_sentences":1},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/1105.5384"}}