{"arxiv_id":"1208.1444","incoming":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"outgoing":{"papers":13,"sentences":18,"groups":[{"kind":"extends","label":"Builds on","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0908.2766","title":"The 3-, 4-, and 5-flavor NNLO Parton from Deep-Inelastic-Scattering Data and at Hadron Colliders","url":"/paper/0908.2766","section":"Introduction","sentence":"These PDFs are obtained from the updated version of the ABKM09 analysis [ref] performed in the fixed-flavor number (FFN) scheme with the number of fermions taken as $n_f=3,4,5$, depending on the process used to constrain the PDFs.","intent_p":0.85,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1011.5790","title":"Heavy-quark deep-inelastic scattering with a running mass","url":"/paper/1011.5790","section":"Introduction","sentence":"However, in the present fit we employ the heavy-quark Wilson coefficients with the $MS$ definition for the $c$- and $b$-quark masses, as suggested in Ref. [ref] .","intent_p":0.89,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":2,"sentences":2,"quotes":[{"arxiv_id":"0911.0884","title":"Combined Measurement and QCD Analysis of the Inclusive ep Scattering Cross Sections at HERA","url":"/paper/0911.0884","section":"Introduction","sentence":"In the present analysis we replace the inclusive neutral-current (NC) DIS data of the H1 and ZEUS experiments by the combined HERA data set, which are obtained from merging those of separate experiments [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1012.4355","title":"Measurement of the Inclusive e{\\pm}p Scattering Cross Section at High Inelasticity y and of the Structure Function FL","url":"/paper/1012.4355","section":"Introduction","sentence":"Finally, we include the H1 data obtained in a special HERA run at reduced collision energy, which are particularly sensitive to the contribution of longitudinal structure function $F_L$ at small $x$ [ref] .","intent_p":0.96,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":7,"sentences":8,"quotes":[{"arxiv_id":"0908.2766","title":"The 3-, 4-, and 5-flavor NNLO Parton from Deep-Inelastic-Scattering Data and at Hadron Colliders","url":"/paper/0908.2766","section":"Introduction","sentence":"This is comparable with our earlier determination $α_s(M_Z)=0.1135±0.0014(exp.)$ [ref] , while the error is improved due to more accurate data employed in the present analysis.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1203.5416","title":"Evaluation of the Strong Coupling Constant alpha_s Using the ATLAS Inclusive Jet Cross-Section Data","url":"/paper/1203.5416","section":"Introduction","sentence":"Moreover, the value of $α_s=0.1151±0.0001 (stata.)±0.0047(sys.)$ extracted from the ATLAS data of Ref. [ref] in the NLO [ref] is in agreement with our results.","intent_p":0.91,"contests_p":null},{"arxiv_id":"1112.6297","title":"Measurement of inclusive jet and dijet production in pp collisions at sqrt(s) = 7 TeV using the ATLAS detector","url":"/paper/1112.6297","section":"Introduction","sentence":"Moreover, the value of $α_s=0.1151±0.0001 (stata.)±0.0047(sys.)$ extracted from the ATLAS data of Ref. [ref] in the NLO [ref] is in agreement with our results.","intent_p":0.91,"contests_p":null},{"arxiv_id":"1106.0208","title":"Measurement of the Inclusive Jet Cross Section in pp Collisions at sqrt(s) = 7 TeV","url":"/paper/1106.0208","section":"Introduction","sentence":"Predictions for the charged-lepton asymmetry and the inclusive jet production cross sections at the energy of LHC are in a good agreement with the first data collected by the CMS and ATLAS experiments [ref] , cf. Figs. 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