{"arxiv_id":"hep-ph/0307179","incoming":{"papers":26,"sentences":31,"groups":[{"kind":"comparison","label":"Compares with it","papers":3,"sentences":5,"quotes":[{"arxiv_id":"2310.06640","title":"Complete Next-to-Leading Order Calculation of Single Inclusive $\\pi^0$ Production in Forward Proton-Nucleus Collisions","url":"/paper/2310.06640","section":"Nuclear modification at parton level","sentence":"This is in contrast to the leading order calculations where the leading order BK evolution changes the asymptotic shape of the dipole amplitude, and consequently one obtains $R_pPb→1$ at moderate transverse momenta $k_⊥∼5…10$ GeV only at the initial condition [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"2012.08562","title":"Saturation effects in SIDIS at very forward rapidities","url":"/paper/2012.08562","section":"Introduction","sentence":"We find that this ratio behaves very similarly to the corresponding ratio in d+Au collisions, as measured at RHIC [ref] and theoretically studied in several publications [ref] : that is, it shows nuclear suppression at low momenta, $k_⊥< Q_s$, and nuclear enhancement at larger momenta, $k_⊥≳Q_s$, with the possible appearance of a (wide) Cronin peak near $k_⊥= Q_s$.","intent_p":0.96,"contests_p":null},{"arxiv_id":"2102.06159","title":"First analysis of world polarized DIS data with small-$x$ helicity evolution","url":"/paper/2102.06159","section":"Constraints from Polarized DIS Data","sentence":"We note that the unpolarized evolution resummation parameter $ln(1/x)$ at $x=0.01$ is approximately equal to the polarized evolution parameter $ln^2 (1/x)$ at $x=0.1$, suggesting comparable accuracy for our helicity evolution with $x_0 = 0.1$ and the unpolarized small-$x$ evolution [ref] with the commonly used value of $x_0=0.01$ [ref] .","intent_p":0.9,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1302.6433","title":"The initial state of heavy-ion collisions","url":"/paper/1302.6433","section":"Single inclusive hadron yields and nuclear modification factors","sentence":"This is the ideal configuration for probing parton saturation effects, and indeed, saturation-based approaches were the only ones to correctly predict the suppression of forward particle production [ref] (as well as the azimuthal decorrelation of forward hadron pairs [ref] , described in the next sub-section).","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1909.02370","title":"Improvement for Color Glass Condensate factorization: single hadron production in pA collisions at next-to-leading order","url":"/paper/1909.02370","section":"Introduction","sentence":"In the following, we will concentrate on single inclusive hadron production at forward rapidity region in nucleon-nucleus (pA) collision [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"2311.02672","title":"Analytic solution of Balitsky-Kovchegov equation with running coupling constant using homogeneous balance method","url":"/paper/2311.02672","section":"Introduction","sentence":"In terms of the numerical solution, the BK equation and its elaborated versions have been deeply investigated [ref] as its simpler nature than the JIMWLK equation.","intent_p":0.84,"contests_p":null},{"arxiv_id":"1608.05293","title":"CGC factorization for forward particle production in proton-nucleus collisions at next-to-leading order","url":"/paper/1608.05293","section":"Introduction","sentence":"Using perturbative QCD, we would like to study particle production in high-energy proton-nucleus ($pA$) collisions in the kinematical regime where the produced particle is semi-hard to hard (meaning that its transverse momenta can be larger than the nuclear saturation momentum $Q_s$, but not much larger) and it propagates at forward rapidity in the proton fragmentation region (that is, it makes a very small angle w.r.t. the collision axis) [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1005.0955","title":"On the gluon spectrum in the glasma","url":"/paper/1005.0955","section":"The $$-factorized approximation","sentence":"This gives an unintegrated gluon distribution $φ()$ (the “WW” distribution, see [ref] ) that is related to the number of gluons as defined in LC quantization and behaves like $ln||$ for small momenta.","intent_p":0.86,"contests_p":null}]}],"unlabelled_sentences":21},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[{"relation":"contradicts","label":"States a conflicting result","papers":[{"arxiv_id":"nucl-th/0307022","url":"/paper/nucl-th/0307022","title":"The Cronin Effect, Quantum Evolution and the Color Glass Condensate","main_claim":"We show that the numerical solution of the classical SU(3) Yang-Mills equations of motion in the McLerran-Venugopalan model for gluon production in central heavy ion collisions leads to a suppresion at low $p_t$ and an enhancement at the intermediate $p_t$ region as compared to peripheral heavy ion and pp collisions at the same energy.","p":0.88}]}],"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/hep-ph/0307179"}}