{"arxiv_id":"2009.03181","incoming":{"papers":3,"sentences":3,"groups":[{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2103.10224","title":"Lepton-Charge and Forward-Backward Asymmetries in Drell-Yan Processes for Precision Electroweak Measurements and New Physics Searches","url":"/paper/2103.10224","section":"Introduction","sentence":"Studies of the impact of $W$ and $Z$ production data on PDFs have recently appeared [ref] based on the ePump package [ref] .","intent_p":0.93,"contests_p":null}]}],"unlabelled_sentences":2},"outgoing":{"papers":38,"sentences":59,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":6,"sentences":6,"quotes":[{"arxiv_id":"1406.3073","title":"Universal Non-perturbative Functions for SIDIS and Drell-Yan Processes","url":"/paper/1406.3073","section":"Updating Error PDFs","sentence":"The theoretical predictions in this work are computed using the ResBos [ref] package at approximate NNLO plus next-to-next-to-leading-logarithm (NNLL) in QCD interactions, in which the canonical scales are used [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ph/0212159","title":"Tevatron Run-1 Z Boson Data and Collins-Soper-Sterman Resummation Formalism","url":"/paper/hep-ph/0212159","section":"Updating Error PDFs","sentence":"The theoretical predictions in this work are computed using the ResBos [ref] package at approximate NNLO plus next-to-next-to-leading-logarithm (NNLL) in QCD interactions, in which the canonical scales are used [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ph/9704258","title":"Soft gluon effects on lepton pairs at hadron colliders","url":"/paper/hep-ph/9704258","section":"Updating Error PDFs","sentence":"The theoretical predictions in this work are computed using the ResBos [ref] package at approximate NNLO plus next-to-next-to-leading-logarithm (NNLL) in QCD interactions, in which the canonical scales are used [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1806.07950","title":"Updating and Optimizing Error PDFs in the Hessian Approach","url":"/paper/1806.07950","section":"Updating Error PDFs","sentence":"Recently, the CTEQ-TEA global analysis group has released a tool named ePump (Error PDF Updating Method Package) [ref] , which can be used to explore the impact of new data on existing PDFs, without perform a full global analysis.","intent_p":0.95,"contests_p":null},{"arxiv_id":"1907.12177","title":"Updating and Optimizing Error PDFs in the Hessian Approach. Part II","url":"/paper/1907.12177","section":"Updating Error PDFs","sentence":"Recently, the CTEQ-TEA global analysis group has released a tool named ePump (Error PDF Updating Method Package) [ref] , which can be used to explore the impact of new data on existing PDFs, without perform a full global analysis.","intent_p":0.95,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":4,"sentences":5,"quotes":[{"arxiv_id":"1607.06495","title":"Measurement of the forward Z boson production cross-section in pp collisions at $\\sqrt{s} = 13$ TeV","url":"/paper/1607.06495","section":"Updating Error PDFs","sentence":"In the ePump study, for the $Z→ℓ^+ℓ^-$ pseudo-data input, the statistical uncertainties are scaled to the 5and 300data samples, separately, by extrapolating the total uncertainty of the LHCb 13publication [ref] to the pseudo-data sample.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1608.01484","title":"Measurement of forward $W\\to e\\nu$ production in $pp$ collisions at $\\sqrt{s}=8\\,$TeV","url":"/paper/1608.01484","section":"Updating Error PDFs","sentence":"Similarly, for the $W^±→ℓ^± ν$ pseudo-data sample, uncertainties are estimated using the LHCb 8publication [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1511.08039","title":"Measurement of forward $W$ and $Z$ boson production in $pp$ collisions at $\\sqrt{s} = 8\\mathrm{\\,Te\\kern -0.1em V}$","url":"/paper/1511.08039","section":"Updating Error PDFs","sentence":"Similarly, for the $W^±→ℓ^± ν$ pseudo-data sample, uncertainties are estimated using the LHCb 8publication [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1903.08726","title":"Observation of $C\\!P$ violation in charm decays","url":"/paper/1903.08726","section":"Introduction","sentence":"In the LHC Run 2 period (2015–2018), the LHCb detector collected more than 5$pp$ collision data [ref] at $=13$.","intent_p":0.87,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1208.5967","title":"Combining QCD and electroweak corrections to dilepton production in FEWZ","url":"/paper/1208.5967","section":"Updating Error PDFs","sentence":"The comparisons between the LHCb 13data and ResBos and FEWZ [ref] predictions are shown in Fig. [ref], with good agreement between data and ResBos prediction.","intent_p":0.92,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1412.6352","title":"LHCb Detector Performance","url":"/paper/1412.6352","section":"Introduction","sentence":"The LHCb detector [ref] is a single-arm forward spectrometer designed for the study of particles containing $b$ or $c$ quarks, covering the pseudorapidity range $2<η<5$.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1203.0275","title":"Precise measurement of the W-boson mass with the CDF II detector","url":"/paper/1203.0275","section":"Introduction","sentence":"In hadron colliders, most physics analyses rely heavily on the understanding of the parton picture of hadronic beam particles, including the precision measurements of the Standard Model (SM) parameters [ref] , and new physics searches.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1701.07240","title":"Measurement of the $W$-boson mass in pp collisions at $\\sqrt{s}=7$ TeV with the ATLAS detector","url":"/paper/1701.07240","section":"Introduction","sentence":"In hadron colliders, most physics analyses rely heavily on the understanding of the parton picture of hadronic beam particles, including the precision measurements of the Standard Model (SM) parameters [ref] , and new physics searches.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1203.0293","title":"Measurement of the W Boson Mass with the D0 Detector","url":"/paper/1203.0293","section":"Introduction","sentence":"In hadron colliders, most physics analyses rely heavily on the understanding of the parton picture of hadronic beam particles, including the precision measurements of the Standard Model (SM) parameters [ref] , and new physics searches.","intent_p":0.93,"contests_p":null}]}],"unlabelled_sentences":43},"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/2009.03181"}}