{"arxiv_id":"1202.4642","incoming":{"papers":3,"sentences":5,"groups":[{"kind":"data_used","label":"Uses its data or values","papers":1,"sentences":2,"quotes":[{"arxiv_id":"1205.5727","title":"On the next-to-next-to-leading order QCD corrections to heavy-quark production in deep-inelastic scattering","url":"/paper/1205.5727","section":"Charm and bottom structure functions at NNLO","sentence":"The dotted and short-dashed curves are the contributions of the LO and NLO coefficient functions to the NNLO results, i.e., these quantities have been calculated using the NNLO values of the strong coupling and the parton distributions as determined in Ref. [ref] .","intent_p":0.94,"contests_p":null}]}],"unlabelled_sentences":3},"outgoing":{"papers":55,"sentences":96,"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":"Taking advantage of the running-mass definition and new massive NNLO corrections we update our ABKM09 PDFs, which were obtained within the fixed-flavor-number (FFN) scheme at NLO and NNLO [ref] , and produce in this way a new PDF set, ABM11.","intent_p":0.92,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":8,"sentences":8,"quotes":[{"arxiv_id":"1011.5790","title":"Heavy-quark deep-inelastic scattering with a running mass","url":"/paper/1011.5790","section":"Introduction","sentence":"The 4(5)-flavor ABM11 PDFs are matched with the 3(4)-flavor ones at the scale of $m_c$ and $m_b$, respectively, employing massive OMEs taken in the running-mass definition [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"hep-ex/0005042","title":"Statistical properties of the estimator using covariance matrix","url":"/paper/hep-ex/0005042","section":"Introduction","sentence":"They are calculated with the standard statistical criterion $Δχ^2=1$ taking into account correlations of the systematic uncertainties in the data within the covariance matrix approach [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1002.3115","title":"W boson production at hadron colliders: the lepton charge asymmetry in NNLO QCD","url":"/paper/1002.3115","section":"Introduction","sentence":"All differential distributions for $W$- and $Z$-boson production are computed with the fully exclusive NNLO program DYNNLO [ref] , which allows to take into account the kinematical cuts imposed in the experiments (cf. Fig. [ref]).","intent_p":1.0,"contests_p":null},{"arxiv_id":"1109.1310","title":"Theory-Data Comparisons for Jet Measurements in Hadron-Induced Processes","url":"/paper/1109.1310","section":"Introduction","sentence":"The NLO QCD corrections [ref] and the partial (soft gluon enhanced) NNLO corrections due to threshold resummation [ref] have been computed with the FastNLO tool [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"hep-ph/0007268","title":"Effects of Higher-Order Threshold Corrections in High-E_T Jet Production","url":"/paper/hep-ph/0007268","section":"Introduction","sentence":"The NLO QCD corrections [ref] and the partial (soft gluon enhanced) NNLO corrections due to threshold resummation [ref] have been computed with the FastNLO tool [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":11,"sentences":14,"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":"Besides, we include into the fit the CC HERA data obtained for the electron and positron beams [ref] .","intent_p":0.96,"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":"With account of these corrections the high-$y$ H1 data [ref] , which are quite sensitive to the contribution from $F_L$ are described pretty well, with the value of $χ^2=137$ for 130 data points.","intent_p":0.84,"contests_p":null},{"arxiv_id":"hep-ex/0105090","title":"Measurement of the neutral current cross section and F2 structure function for deep inelastic e+p scattering at HERA","url":"/paper/hep-ex/0105090","section":"Introduction","sentence":"Firstly, the separate H1 [ref] and ZEUS [ref] data sets on the NC inclusive SFs are replaced by much more accurate combined HERA data [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ex/0012053","title":"Deep-Inelastic Inclusive ep Scattering at Low x and a Determination of alpha_s","url":"/paper/hep-ex/0012053","section":"Introduction","sentence":"Firstly, the separate H1 [ref] and ZEUS [ref] data sets on the NC inclusive SFs are replaced by much more accurate combined HERA data [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ph/9610231","title":"Measurement of the proton and deuteron structure functions, F2p and F2d, and of the ratio sigma(L)/sigma(T)","url":"/paper/hep-ph/9610231","section":"Introduction","sentence":"Also we employ the fixed-target inclusive DIS data obtained in the NMC [ref] , the BCDMS [ref] , and the SLAC experiments [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":6,"sentences":12,"quotes":[{"arxiv_id":"1011.5790","title":"Heavy-quark deep-inelastic scattering with a running mass","url":"/paper/1011.5790","section":"Introduction","sentence":"To demonstrate that the treatment of the charm production within the FFN scheme is applicable at that large transverse momentum we compared the predictions based on the variant of the NNLO ABKM09 fit performed with the running-mass scheme [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"1101.1300","title":"Impact of Heavy Quark Masses on Parton Distributions and LHC Phenomenology","url":"/paper/1101.1300","section":"Introduction","sentence":"The NNLO predictions based on the MSTW [ref] and JR09 [ref] PDFs are in a good agreement with ours and with the H1 data, while the NLO NN21 [ref] predictions systematically undershoot the data.","intent_p":0.99,"contests_p":null},{"arxiv_id":"0810.4274","title":"Dynamical NNLO parton distributions","url":"/paper/0810.4274","section":"Introduction","sentence":"The NNLO predictions based on the MSTW [ref] and JR09 [ref] PDFs are in a good agreement with ours and with the H1 data, while the NLO NN21 [ref] predictions systematically undershoot the data.","intent_p":0.99,"contests_p":null},{"arxiv_id":"0901.0002","title":"Parton distributions for the LHC","url":"/paper/0901.0002","section":"Introduction","sentence":"The NNLO predictions based on the MSTW [ref] and JR09 [ref] PDFs are in a good agreement with ours and with the H1 data, while the NLO NN21 [ref] predictions systematically undershoot the data.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1202.2281","title":"Parton distribution functions and benchmark cross sections at NNLO","url":"/paper/1202.2281","section":"Introduction","sentence":"Many other aspects of our analysis, which may affect the value of $α_s$, are also different from [ref] : basic relations for the DIS cross sections, data normalization, etc, cf. Ref. [ref] for a detailed discussion.","intent_p":0.91,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites as support","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1011.5790","title":"Heavy-quark deep-inelastic scattering with a running mass","url":"/paper/1011.5790","section":"Introduction","sentence":"The massive Wilson coefficients re-calculated in terms of the running mass also demonstrate improved perturbative stability and the reduced renormalization/factorization scale sensitivity at the HERA kinematics [ref] .","intent_p":0.99,"contests_p":null},{"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":"Furthermore the results of the PDF-analysis are not sensitive to the choice of either the VFN scheme as the BMSN prescription or the FFN scheme [ref] .","intent_p":0.98,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":5,"sentences":7,"quotes":[{"arxiv_id":"1008.3347","title":"The O(\\alpha_s^3) Massive Operator Matrix Elements of O(n_f) for the Structure Function F_2(x,Q^2) and Transversity","url":"/paper/1008.3347","section":"Introduction","sentence":"The matching conditions between 3- and 4-flavor schemes are known up to the second order in $α_s$ [ref] and the first third-order corrections are also available [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"0901.0669","title":"The Gluonic Operator Matrix Elements at O(\\alpha_s^2) for DIS Heavy Flavor Production","url":"/paper/0901.0669","section":"Introduction","sentence":"The matching conditions between 3- and 4-flavor schemes are known up to the second order in $α_s$ [ref] and the first third-order corrections are also available [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"hep-ph/9612398","title":"Charm electroproduction viewed in the variable-flavour number scheme versus fixed-order perturbation theory","url":"/paper/hep-ph/9612398","section":"Introduction","sentence":"The matching conditions between 3- and 4-flavor schemes are known up to the second order in $α_s$ [ref] and the first third-order corrections are also available [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"0904.3563","title":"Mellin Moments of the {$O(\\alpha_s^3$)} Heavy Flavor Contributions to unpolarized Deep-Inelastic Scattering at $Q^2 \\gg m^2$ and Anomalous Dimensions","url":"/paper/0904.3563","section":"Introduction","sentence":"The matching conditions between 3- and 4-flavor schemes are known up to the second order in $α_s$ [ref] and the first third-order corrections are also available [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"1201.6180","title":"Effect of changes of variable flavor number scheme on parton distribution functions and predicted cross sections","url":"/paper/1201.6180","section":"Introduction","sentence":"In cases the smoothness is achieved by introducing empirical parameter(s), which control dumping of the massless VFN term at small $Q^2$ [ref] .","intent_p":0.8,"contests_p":null}]}],"unlabelled_sentences":52},"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/1202.4642"}}