{"arxiv_id":"2308.10136","incoming":{"papers":1,"sentences":10,"groups":[{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2406.12425","title":"Accessing the stringy structure of proton in the framework of Color Glass Condensate","url":"/paper/2406.12425","section":"Dipole-proton cross section","sentence":"This outcome is coincident with the results in Ref. 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[ref] , since it successfully describes the vector meson production data at HERA.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1607.01711","title":"Revealing proton shape fluctuations with incoherent diffraction at high energy","url":"/paper/1607.01711","section":"Hot spot model","sentence":"We shall include the saturation scale fluctuations by following Ref. [ref] , in which the saturation scale fluctuates in terms of P(lnQ_s^2/⟨Q_s^2⟩)=1/√(2π)σexp[-ln^2Q_s^2/⟨Q_s^2⟩/2σ^2].","intent_p":0.89,"contests_p":null},{"arxiv_id":"1812.02548","title":"Collinearly improved kernel suppresses Coulomb tails in the impact-parameter dependent Balitsky-Kovchegov evolution","url":"/paper/1812.02548","section":"conclusions and discussions","sentence":"Moreover, our calculations can be improved by performing the QCD evolution (dipole scattering amplitude) via the collinearly-improved Balitsky-Kovchegove equation whose Coulomb tails are strongly suppressed by the resumed kernel and can give the numerical version of the impact parameter dependent dipole scattering amplitude [ref] , which is our next step work.","intent_p":0.83,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1607.01711","title":"Revealing proton shape fluctuations with incoherent diffraction at high energy","url":"/paper/1607.01711","section":"Introduction","sentence":"The average width is extracted from the exclusive $J/Ψ$ production data in Ref. 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