{"arxiv_id":"1502.08032","incoming":{"papers":7,"sentences":9,"groups":[{"kind":"comparison","label":"Compares with it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1611.07770","title":"Neutrino-Nucleus Cross Sections for Oscillation Experiments","url":"/paper/1611.07770","section":"Flux-integrated cross section","sentence":"Here, theoretical calculation by GiBUU is compared with MiniBooNE [ref] (left) and MINERvA data [ref] (right).","intent_p":0.92,"contests_p":null},{"arxiv_id":"1406.6415","title":"Charged Pion Production in $\\nu_\\mu$ Interactions on Hydrocarbon at $\\langle E_{\\nu}\\rangle$= 4.0 GeV","url":"/paper/1406.6415","section":"Models","sentence":"Predictions from the GiBUU model can be found in Refs. [ref] .","intent_p":0.86,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1909.13562","title":"Low-energy axial-vector transitions from decuplet to octet baryons","url":"/paper/1909.13562","section":"Introduction and summary","sentence":"One of the interesting processes of neutrino-nucleon scattering is the production of the lowest-lying Delta state [ref] .","intent_p":0.97,"contests_p":null}]}],"unlabelled_sentences":6},"outgoing":{"papers":41,"sentences":77,"groups":[{"kind":"contests","label":"Contests","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1411.6637","title":"Comparison of the ANP model with the data for neutrino induced single pion production from the MiniBooNE and MINER$\\nu$A experiments","url":"/paper/1411.6637","section":"Method","sentence":"This model does not describe the $π-N-Δ$ dynamics correctly and indeed the authors of [ref] themselves ascribe the failure of the model to describe the MINER$ν$A data to the absence of all pion-nucleon interactions, except for absorption, in that model.","intent_p":0.97,"contests_p":0.94}]},{"kind":"extends","label":"Builds on","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1205.1061","title":"Neutrino- and antineutrino-induced reactions with nuclei between 1 and 50 GeV","url":"/paper/1205.1061","section":"Introduction","sentence":"While first results were already contained in [ref] in the present paper now a detailed comparison with MINER$ν$A data is performed using their flux and invariant mass cuts.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1402.0297","title":"Reaction Mechanisms at MINER$\\nu$A","url":"/paper/1402.0297","section":"Introduction","sentence":"While first results were already contained in [ref] in the present paper now a detailed comparison with MINER$ν$A data is performed using their flux and invariant mass cuts.","intent_p":0.94,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":6,"sentences":6,"quotes":[{"arxiv_id":"1106.1344","title":"Transport-theoretical Description of Nuclear Reactions","url":"/paper/1106.1344","section":"Method","sentence":"In GiBUU these resonances are treated explicitly; they become excited and then are being propagated until they decay or collide with other nucleons; this is described in some detail in [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"nucl-th/0601103","title":"Charged Current Neutrino Nucleus Interactions at Intermediate Energies","url":"/paper/nucl-th/0601103","section":"Method","sentence":"The production cross section at fixed neutrino energy is then given by (cf. [ref] where all the details can be found) [equation] Here $f_corr$ is a flux correction factor, $f_corr = (k ·p)/(k^0p^0)$; $k$ and $p$ denote the four-momenta of the neutrino and nucleon momentum, respectively. $𝒫_PB(𝐫,𝐩)$ describes the Pauli-blocking and the factor $F_π(𝐪_π, 𝐫)$ in ([ref]) describes the effects of all the FSI contained in GiBUU.","intent_p":0.9,"contests_p":null},{"arxiv_id":"nucl-th/0607016","title":"Pion induced double charge exchange reactions in the Delta resonance region","url":"/paper/nucl-th/0607016","section":"Method","sentence":"Therefore, for the FSI process $π+ N →Δ→π+ N$ a more sophisticated parametrization of the $p$-wave behavior of the $Δ$ decay is used as explained in detail in [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"1007.0925","title":"One pion production in neutrino reactions: including non-resonant background","url":"/paper/1007.0925","section":"Method","sentence":"For the background contribution a form taken from an effective field theory treatment of pion production up the $Δ$ resonance region [ref] is used.","intent_p":0.95,"contests_p":null},{"arxiv_id":"hep-ph/0701149","title":"Weak Pion Production off the Nucleon","url":"/paper/hep-ph/0701149","section":"Method","sentence":"For the background contribution a form taken from an effective field theory treatment of pion production up the $Δ$ resonance region [ref] is used.","intent_p":0.95,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":1,"sentences":2,"quotes":[{"arxiv_id":"1406.6415","title":"Charged Pion Production in $\\nu_\\mu$ Interactions on Hydrocarbon at $\\langle E_{\\nu}\\rangle$= 4.0 GeV","url":"/paper/1406.6415","section":"Summary and Conclusion","sentence":"In this paper primarily the recent MINER$ν$A data on charged pion production [ref] were analyzed.","intent_p":0.96,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":7,"sentences":7,"quotes":[{"arxiv_id":"1406.6415","title":"Charged Pion Production in $\\nu_\\mu$ Interactions on Hydrocarbon at $\\langle E_{\\nu}\\rangle$= 4.0 GeV","url":"/paper/1406.6415","section":"Charged pion production in the neutrino beam","sentence":"In Fig. [ref] the calculated kinetic energy distribution for the sum of $π^+$ and $π^-$ is shown in comparison with the data [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1011.3572","title":"Measurement of Neutrino-Induced Charged-Current Charged Pion Production Cross Sections on Mineral Oil at E$_{\\nu}\\sim 1~\\textrm{GeV}$","url":"/paper/1011.3572","section":"Method","sentence":"The extensive pion production data from the MiniBooNE experiment [ref] obtained on a CH$_2$ target are consistently higher than the ones calculated within GiBUU, both for the ANL and – less so – for the BNL input cross sections [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1010.3264","title":"Measurement of $\\nu_\\mu$-induced charged-current neutral pion production cross sections on mineral oil at $E_\\nu\\in0.5-2.0$ GeV","url":"/paper/1010.3264","section":"Method","sentence":"The extensive pion production data from the MiniBooNE experiment [ref] obtained on a CH$_2$ target are consistently higher than the ones calculated within GiBUU, both for the ANL and – less so – for the BNL input cross sections [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1210.4717","title":"Pion production in the MiniBooNE experiment","url":"/paper/1210.4717","section":"Method","sentence":"The extensive pion production data from the MiniBooNE experiment [ref] obtained on a CH$_2$ target are consistently higher than the ones calculated within GiBUU, both for the ANL and – less so – for the BNL input cross sections [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1304.1320","title":"Single pion production in neutrino nucleus scattering","url":"/paper/1304.1320","section":"Method","sentence":"The extensive pion production data from the MiniBooNE experiment [ref] obtained on a CH$_2$ target are consistently higher than the ones calculated within GiBUU, both for the ANL and – less so – for the BNL input cross sections [ref] .","intent_p":0.89,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1402.0297","title":"Reaction Mechanisms at MINER$\\nu$A","url":"/paper/1402.0297","section":"Summary and Conclusion","sentence":"It was shown in [ref] that the flux cuts used by the MINER$ν$A experiment can significantly distort the event rates, requiring a fairly large and generator-dependent correction through energy-migration matrices.","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1010.3264","title":"Measurement of $\\nu_\\mu$-induced charged-current neutral pion production cross sections on mineral oil at $E_\\nu\\in0.5-2.0$ GeV","url":"/paper/1010.3264","section":"Introduction","sentence":"Over the last few years valuable insight into the neutrino-induced pion production on nuclei at lower energies has been obtained mainly from the MiniBooNE experiment [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1210.4717","title":"Pion production in the MiniBooNE experiment","url":"/paper/1210.4717","section":"Introduction","sentence":"Over the last few years valuable insight into the neutrino-induced pion production on nuclei at lower energies has been obtained mainly from the MiniBooNE experiment [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1304.1320","title":"Single pion production in neutrino nucleus scattering","url":"/paper/1304.1320","section":"Introduction","sentence":"Over the last few years valuable insight into the neutrino-induced pion production on nuclei at lower energies has been obtained mainly from the MiniBooNE experiment [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1011.3572","title":"Measurement of Neutrino-Induced Charged-Current Charged Pion Production Cross Sections on Mineral Oil at E$_{\\nu}\\sim 1~\\textrm{GeV}$","url":"/paper/1011.3572","section":"Introduction","sentence":"Over the last few years valuable insight into the neutrino-induced pion production on nuclei at lower energies has been obtained mainly from the MiniBooNE experiment [ref] .","intent_p":0.96,"contests_p":null}]}],"unlabelled_sentences":54},"claims":[{"relation":"same_result","label":"States the same result","papers":[{"arxiv_id":"1107.5944","url":"/paper/1107.5944","title":"Neutrino nucleus reactions at high energies within the GiBUU model","main_claim":"It is shown, that final state interaction can noticeably change the spectra of the outgoing hadrons.","p":0.92}]}],"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/1502.08032"}}