{"arxiv_id":"2406.12425","incoming":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"outgoing":{"papers":53,"sentences":96,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":2,"sentences":3,"quotes":[{"arxiv_id":"1603.04349","title":"Evidence of strong proton shape fluctuations from incoherent diffraction","url":"/paper/1603.04349","section":"Dipole-proton cross section","sentence":"The density profile of the gluon tube, which connects the constituent quarks and Fermat point of the quark triangle, also has a Gaussian distribution and can be obtained by integration over the longitudinal direction [ref] T_t(b)=1/2πB_t∫db_zexp(-b^2+b_z^2/2B_t),","intent_p":0.8,"contests_p":null},{"arxiv_id":"1607.01711","title":"Revealing proton shape fluctuations with incoherent diffraction at high energy","url":"/paper/1607.01711","section":"Dipole-proton cross section","sentence":"The density profile of the gluon tube, which connects the constituent quarks and Fermat point of the quark triangle, also has a Gaussian distribution and can be obtained by integration over the longitudinal direction [ref] T_t(b)=1/2πB_t∫db_zexp(-b^2+b_z^2/2B_t),","intent_p":0.8,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1304.5162","title":"Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA","url":"/paper/1304.5162","section":"Comparisons between improved stringy proton and hot spot models","sentence":"The coherent and incoherent differential cross sections of the $J/Ψ$ production as a function of transverse momentum transfer $t$ in $γ^*+p$ DIS are present in Fig.[ref], where the experimental data are taken from H1 and ZEUS Collaborations at HERA [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"hep-ex/0201043","title":"Exclusive photoproduction of J/psi mesons at HERA","url":"/paper/hep-ex/0201043","section":"Comparisons between improved stringy proton and hot spot models","sentence":"The coherent and incoherent differential cross sections of the $J/Ψ$ production as a function of transverse momentum transfer $t$ in $γ^*+p$ DIS are present in Fig.[ref], where the experimental data are taken from H1 and ZEUS Collaborations at HERA [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"hep-ex/0205081","title":"Measurement of proton-dissociative diffractive photoproduction of vector mesons at large momentum transfer at HERA","url":"/paper/hep-ex/0205081","section":"Comparisons between improved stringy proton and hot spot models","sentence":"The coherent and incoherent differential cross sections of the $J/Ψ$ production as a function of transverse momentum transfer $t$ in $γ^*+p$ DIS are present in Fig.[ref], where the experimental data are taken from H1 and ZEUS Collaborations at HERA [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"hep-ex/0510016","title":"Elastic J/Psi Production at HERA","url":"/paper/hep-ex/0510016","section":"Comparisons between improved stringy proton and hot spot models","sentence":"The coherent and incoherent differential cross sections of the $J/Ψ$ production as a function of transverse momentum transfer $t$ in $γ^*+p$ DIS are present in Fig.[ref], where the experimental data are taken from H1 and ZEUS Collaborations at HERA [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":4,"sentences":4,"quotes":[{"arxiv_id":"2102.00110","title":"The mass radius of the proton","url":"/paper/2102.00110","section":"Comparisons between improved stringy proton and hot spot models","sentence":"When one calculates the root mean square radius of the proton $r_p=√(2(B_p+B_u/d))$, and gets $r_p=0.55 fm$, which is in agreement with the one obtained by fitting to the data from the GlueX Collaboration at Jefferson Lab [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1905.10811","title":"First measurement of near-threshold J/$\\psi $ exclusive photoproduction off the proton","url":"/paper/1905.10811","section":"Comparisons between improved stringy proton and hot spot models","sentence":"When one calculates the root mean square radius of the proton $r_p=√(2(B_p+B_u/d))$, and gets $r_p=0.55 fm$, which is in agreement with the one obtained by fitting to the data from the GlueX Collaboration at Jefferson Lab [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1607.01711","title":"Revealing proton shape fluctuations with incoherent diffraction at high energy","url":"/paper/1607.01711","section":"Comparisons between improved stringy proton and hot spot models","sentence":"Finally, we would like to mention that the width parameters ($B_p=3.0 GeV^-2$, $B_u=1.0 GeV^-2$, and $B_d=1.0 GeV^-2$) resulting from the ISP model are consistent with ones coming from the HS model [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"2308.10136","title":"Imaging constituent quark shape of proton with exclusive vector meson production at HERA","url":"/paper/2308.10136","section":"Dipole-proton cross section","sentence":"This outcome is coincident with the results in Ref. [ref] where the up quark inspired hot spot width is larger or equal to the down quark inspired hot spot width.","intent_p":0.92,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":25,"sentences":39,"quotes":[{"arxiv_id":"hep-ph/0109115","title":"Nonlinear Gluon Evolution in the Color Glass Condensate: II","url":"/paper/hep-ph/0109115","section":"Dipole-proton cross section","sentence":"In the CGC framework, the rapidity (or $x$) evolution of the dipole scattering amplitude is governed by the JIMWLK[The JIMWLK is the abbreviation of Jalilian-Marian, Iancu, McLerran, Weigert, Leonidov, Kovner.] evolution equation [ref] , which can be reduced to a closed Balitsky-Kovchegov (BK) equation in the mean field approximation [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"hep-ph/0011241","title":"Nonlinear Gluon Evolution in the Color Glass Condensate: I","url":"/paper/hep-ph/0011241","section":"Dipole-proton cross section","sentence":"In the CGC framework, the rapidity (or $x$) evolution of the dipole scattering amplitude is governed by the JIMWLK[The JIMWLK is the abbreviation of Jalilian-Marian, Iancu, McLerran, Weigert, Leonidov, Kovner.] evolution equation [ref] , which can be reduced to a closed Balitsky-Kovchegov (BK) equation in the mean field approximation [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"hep-ph/9706377","title":"The Wilson renormalization group for low x physics: towards the high density regime","url":"/paper/hep-ph/9706377","section":"Dipole-proton cross section","sentence":"In the CGC framework, the rapidity (or $x$) evolution of the dipole scattering amplitude is governed by the JIMWLK[The JIMWLK is the abbreviation of Jalilian-Marian, Iancu, McLerran, Weigert, Leonidov, Kovner.] evolution equation [ref] , which can be reduced to a closed Balitsky-Kovchegov (BK) equation in the mean field approximation [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"hep-ph/9905214","title":"Unitarization of the BFKL Pomeron on a Nucleus","url":"/paper/hep-ph/9905214","section":"Dipole-proton cross section","sentence":"In the CGC framework, the rapidity (or $x$) evolution of the dipole scattering amplitude is governed by the JIMWLK[The JIMWLK is the abbreviation of Jalilian-Marian, Iancu, McLerran, Weigert, Leonidov, Kovner.] evolution equation [ref] , which can be reduced to a closed Balitsky-Kovchegov (BK) equation in the mean field approximation [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"hep-ph/9701284","title":"The BFKL Equation from the Wilson Renormalization Group","url":"/paper/hep-ph/9701284","section":"Dipole-proton cross section","sentence":"In the CGC framework, the rapidity (or $x$) evolution of the dipole scattering amplitude is governed by the JIMWLK[The JIMWLK is the abbreviation of Jalilian-Marian, Iancu, McLerran, Weigert, Leonidov, Kovner.] evolution equation [ref] , which can be reduced to a closed Balitsky-Kovchegov (BK) equation in the mean field approximation [ref] .","intent_p":0.88,"contests_p":null}]}],"unlabelled_sentences":46},"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/2406.12425"}}