{"arxiv_id":"1101.2672","incoming":{"papers":43,"sentences":55,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":4,"sentences":5,"quotes":[{"arxiv_id":"1408.0278","title":"Hadroproduction of t anti-t pair with two isolated photons with PowHel","url":"/paper/1408.0278","section":"Introduction","sentence":"The essence of the new method of predicting cross sections for processes with isolated photons is to introduce generation isolation [ref] and generation cuts [ref] during event generation that are sufficiently small so that predictions at the hadron level obtained with physical cuts and isolation do not depend on them.","intent_p":0.85,"contests_p":null},{"arxiv_id":"1405.5859","title":"Hadroproduction of $W^+ W^- b \\bar{b}$ at NLO accuracy matched with shower Monte Carlo programs","url":"/paper/1405.5859","section":"Introduction","sentence":"For this purpose we choose the simplest process, hadroproduction and the POWHEG method [ref] as implemented in the framework [ref] which is based on the [ref] and [ref] programs.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1406.2324","title":"Hadroproduction of t anti-t pair in association with an isolated photon at NLO accuracy matched with parton shower","url":"/paper/1406.2324","section":"Introduction","sentence":"In a series of papers we combined the with the package [ref] into to make predictions for the hadroproduction of a -pair in association with a hard boson (scalar [ref] , pseudoscalar [ref] , vector [ref] or jet [ref] ).","intent_p":0.81,"contests_p":null},{"arxiv_id":"2112.11451","title":"Theory input for $t\\bar{t}j$ experimental analyses at the LHC","url":"/paper/2112.11451","section":"Introduction","sentence":"The combination of the NLO $tt̅j$ calculation and a parton shower (PS) was first presented in [ref] using hard scattering amplitudes from HELAC-NLO [ref] and the PS matching method implemented in the POWHEG-BOX [ref] .","intent_p":0.83,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1103.2757","title":"Explaining the t tbar forward-backward asymmetry without dijet or flavor anomalies","url":"/paper/1103.2757","section":"LHC signals: $uc$ resonance and $pp→j$","sentence":"Comparing with recent predictions for the $j$ distributions at the 7 TeV LHC [ref] , we find that simply cutting on $p_T$ of the hardest jet, our signal is somewhat smaller than the SM background.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1111.4991","title":"Top quark pair production in association with a jet: QCD corrections and jet radiation in top quark decays","url":"/paper/1111.4991","section":"Phenomenological results","sentence":"Note, however, that the cross-section computed in Ref. [ref] seems closer to the contribution that we identify as “jet radiation in production”.","intent_p":0.93,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":11,"sentences":11,"quotes":[{"arxiv_id":"1405.5859","title":"Hadroproduction of $W^+ W^- b \\bar{b}$ at NLO accuracy matched with shower Monte Carlo programs","url":"/paper/1405.5859","section":"Introduction","sentence":"Another line of research was to make improvements by implementing the production of t-quarks at the NLO accuracy and match those to shower Monte Carlo programs (SMCs) [ref] .","intent_p":0.84,"contests_p":null},{"arxiv_id":"1502.00925","title":"Matching the Nagy-Soper parton shower at next-to-leading order","url":"/paper/1502.00925","section":"$tt̅ j$ production at the LHC with next-to-leading order matching","sentence":"Matching to a parton shower has been first considered in Ref. [ref] using the method [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"1803.00950","title":"Multi-jet merged top-pair production including electroweak corrections","url":"/paper/1803.00950","section":"Introduction","sentence":"Particle-level Monte Carlo generators matching NLO QCD matrix elements to parton showers have been available for quite some time for inclusive production [ref] and since recently for [ref] and $tt̅+2$ jet [ref] production.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1607.06934","title":"Next-to-leading order QCD predictions for top-quark pair production with up to three jets","url":"/paper/1607.06934","section":"Introduction","sentence":"Predictions for top-quark pair production in association with up to two jets are available at the next–­to–leading order (NLO) [ref] , and NLO calculations for inclusive top-quark pair production and in association with up to one or two jets were matched to parton showers in order to provide predictions at the particle level [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"2203.07344","title":"Top-quark mass extraction from $t\\bar{t}j +X$ events at the LHC: theory predictions","url":"/paper/2203.07344","section":"Theoretical framework","sentence":"been matched [ref] with the parton shower implementations available in different Shower Monte Carlo codes, by using different matching methods.","intent_p":0.84,"contests_p":null}]}],"unlabelled_sentences":37},"outgoing":{"papers":2,"sentences":2,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1009.5594","title":"Vector boson plus one jet production in POWHEG","url":"/paper/1009.5594","section":"Checks","sentence":"Another way of treating the same problem, also implemented in the , is to use a suppression factor on the underlying Born configuration [ref] .","intent_p":0.92,"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/1101.2672"}}