{"arxiv_id":"1312.2150","incoming":{"papers":3,"sentences":4,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1905.10419","title":"Rescattering effects in antiproton-induced exclusive $J/\\psi$ and $\\psi^\\prime$ production on the deuteron","url":"/paper/1905.10419","section":"The model","sentence":"We employ in our calculations the generalized eikonal approximation to the multiple-scattering theory [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1601.00189","title":"Color transparency in $\\pi^-$-induced dilepton production on nuclei","url":"/paper/1601.00189","section":"Model","sentence":"The amplitude of Fig. [ref] can be calculated within the generalized eikonal approximation [ref] .","intent_p":0.99,"contests_p":null}]}],"unlabelled_sentences":2},"outgoing":{"papers":9,"sentences":17,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":2,"sentences":4,"quotes":[{"arxiv_id":"nucl-th/9803034","title":"J/\\Psi production, $\\chi$ polarization and Color Fluctuations","url":"/paper/nucl-th/9803034","section":"Transition amplitudes $χ_J_1 N →χ_J N$","sentence":"Following [ref] we decompose the internal $cc̅$ wave function of the physical $χ_Jν$-charmonium state in the basis of wave functions with fixed orbital ($L_z$) and spin ($S_z$) magnetic quantum numbers as [equation] where $z$-axis is directed along the charmonium momentum in the target nucleus rest frame (Fermi motion is neglected here). $⟨1L_z;1S_z|Jν⟩$ are the Clebsch-Gordan coefficients.","intent_p":0.95,"contests_p":null},{"arxiv_id":"nucl-th/9603018","title":"Feynman Graphs and Generalized Eikonal Approach to High Energy Knock-Out Processes","url":"/paper/nucl-th/9603018","section":"Summary","sentence":"We have used the multiple scattering Feynman diagram formalism in the GEA-approach of Refs. [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":3,"sentences":4,"quotes":[{"arxiv_id":"nucl-th/9803034","title":"J/\\Psi production, $\\chi$ polarization and Color Fluctuations","url":"/paper/nucl-th/9803034","section":"Transition amplitudes $χ_J_1 N →χ_J N$","sentence":"The following values have been obtained in [ref] : $σ_0=6.8$ mb and $σ_±1= 15.9$ mb.","intent_p":0.8,"contests_p":null},{"arxiv_id":"0806.4412","title":"Recent observation of short range nucleon correlations in nuclei and their implications for the structure of nuclei and neutron stars","url":"/paper/0806.4412","section":"Occupation numbers","sentence":"In the present work we will use a simple expression for $n(𝐗,𝐩)$, which is based on the local Fermi distribution but takes into account the corrections due to the short range NN correlations (SRC): [equation] Here $ρ_p(𝐗)$ is the proton density; $p_F(𝐗)=(3π^2ρ_p)^1/3$ is the proton Fermi momentum; and $P_2 ≃0.25$ is the proton fraction above Fermi surface [ref] .","intent_p":0.82,"contests_p":null},{"arxiv_id":"1303.0236","title":"Charmonium production in antiproton-nucleus reactions at low energies","url":"/paper/1303.0236","section":"Occupation numbers","sentence":"The density distributions of protons and neutrons have been taken in the two-parameter Fermi parameterization as described in [ref] .","intent_p":0.87,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":1,"quotes":[{"arxiv_id":"hep-ph/0007111","title":"Photoproduction of Charmonia and Total Charmonium-Proton Cross Sections","url":"/paper/hep-ph/0007111","section":"Introduction","sentence":"Qualitatively similar results were obtained later in Ref. [ref] , however, with somewhat different absolute values of the charmonium-nucleon cross sections.","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":2,"sentences":2,"quotes":[{"arxiv_id":"nucl-th/9803034","title":"J/\\Psi production, $\\chi$ polarization and Color Fluctuations","url":"/paper/nucl-th/9803034","section":"Introduction","sentence":"This was first predicted in Ref. [ref] , where the cross sections of the charmonium- and bottomonium-nucleon interaction have been calculated on the basis of the QCD factorization theorem and the nonrelativistic quarkonium model.","intent_p":0.88,"contests_p":null},{"arxiv_id":"0903.3905","title":null,"url":"/paper/0903.3905","section":"Numerical results","sentence":"The PANDA experimental program [ref] already includes the studies of the $p̅ p →χ_c →J/ψγ→e^+ e^- γ$ reaction.","intent_p":0.84,"contests_p":null}]}],"unlabelled_sentences":6},"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/1312.2150"}}