{"arxiv_id":"1011.1895","incoming":{"papers":44,"sentences":69,"groups":[{"kind":"contests","label":"Contests it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1607.00832","title":"CGC/saturation approach: a new impact-parameter dependent model in the next-to-leading order of perturbative QCD","url":"/paper/1607.00832","section":"Fitting $F_2$ and values of the parameters","sentence":"However, the main complication of this model is that it gives rather a large value of $Q_0^2$ (see qs) which is in sharp contradiction to the value of the saturation momentum, from all other model description of the experimental data [ref] .","intent_p":0.75,"contests_p":0.74}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1803.11093","title":"Event engineering studies for heavy flavor production and hadronization in high multiplicity hadron-hadron and hadron-nucleus collisions","url":"/paper/1803.11093","section":"Results for $D$-meson and $J/ψ$ production","sentence":"The latter is computed in a $k_⊥$ factorized approximation to the CGC EFT [ref] as shown in Appendix [ref].","intent_p":0.97,"contests_p":null},{"arxiv_id":"1706.07617","title":"A CGC/saturation approach for angular correlations in proton-proton scattering","url":"/paper/1706.07617","section":"Modification to also include DIS","sentence":"[ref] : we change $γ̅$ in T γ̅ =1 - γ_cr → 1 - γ_cr - 1/2 κ λ Y ln r^2 Q^2_sb = 0.63 - 1/2 κ λ Y ln r^2 Q^2_sb where $κ = χ”γ_cr/χ'γ_cr= 9.8$. $χγ$ is the BFKL kernel which has the foliowing form χγ = 2 ψ(1) - ψ(γ) - ψ( 1 - γ) χγ_cr/1 - γ_cr = d χγ/ d γ|_γ= γ_cr where $ψ(z) = d Γ(z)/d z$ is the Euler $ψ$-function (see Ref. [ref] formula 8.360).","intent_p":0.81,"contests_p":null},{"arxiv_id":"1511.07452","title":"Diffractive Dijet Production in Deep Inelastic Scattering and Photon-Hadron Collisions in the Color Glass Condensate","url":"/paper/1511.07452","section":"Numerical results","sentence":"We use two well-known impact-parameter dependent saturation models, the so-called IP-Sat [ref] and the b-CGC [ref] models which both have been very successful in phenomenological applications from HERA to the Relativistic Heavy Ion Collider (RHIC) and the LHC, see for example [ref] .","intent_p":0.9,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1111.3031","title":"Gluon saturation in $pA$ collisions at the LHC: KLN model predictions for hadron multiplicities","url":"/paper/1111.3031","section":"Introduction","sentence":"The quantity $k$ which characterizes the fluctuations in the saturation approach has been estimated as be [ref]","intent_p":0.94,"contests_p":null},{"arxiv_id":"1210.3890","title":"Evidence for BFKL and saturation dynamics from di-hadron spectra at the LHC","url":"/paper/1210.3890","section":"Introduction","sentence":"One important source of uncertainty is due to the non-perturbative constant[$ζ$ is constrained by numerical computations [ref] and fits to the n-particle p+p multiplicity distribution [ref] to be $ζ∼1/6$.","intent_p":0.95,"contests_p":null},{"arxiv_id":"1509.04410","title":"Energy dependence of the ridge in high multiplicity proton-proton collisions","url":"/paper/1509.04410","section":"Introduction","sentence":"This leaves only the parameter $ζ$, which was extracted previously by an independent $$ factorization analysis of data on $n$-particle multiplicity distributions [ref] and estimated to be $ζ=1/6$.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1201.2658","title":"Azimuthal collimation of long range rapidity correlations by strong color fields in high multiplicity hadron-hadron collisions","url":"/paper/1201.2658","section":"Introduction","sentence":"Fits to p+p multiplicity distributions for a range of energies at the LHC and A+A multiplicity distributions at RHIC obtained $ζ=1/6$ [ref] .","intent_p":0.93,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":4,"sentences":5,"quotes":[{"arxiv_id":"1508.02544","title":"CGC/saturation approach: a new impact-parameter dependent model","url":"/paper/1508.02544","section":"Conclusions","sentence":"The weak statement is nevertheless stronger than the one that we can make from the models of Refs. [ref] : shadowing corrections are, perhaps, needed to describe the experimental data.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1802.06344","title":"CGC/saturation approach: an impact-parameter dependent model for diffraction production in DIS","url":"/paper/1802.06344","section":"Introduction.","sentence":"This formula exhibits the main features of the DIS amplitude , given in Refs. [ref] , but it is different from the interpolation procedure that have been used in numerous attempts to build a such model in Refs. [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"1106.1375","title":"Single Spin Asymmetry Scaling in the Forward Rapidity Region at RHIC","url":"/paper/1106.1375","section":"Transverse Momentum Dependent Geometric Scaling","sentence":"Similar geometric scaling for inclusive hadron production at central rapidity has been observed in [ref] , where it is the differential cross section alone exhibits the geometric scaling.","intent_p":0.82,"contests_p":null},{"arxiv_id":"1205.3223","title":"Holographic Pomeron: Saturation and DIS","url":"/paper/1205.3223","section":"Confining","sentence":"Also note the non-trivial dependence on the impact parameter in the scattering amplitude or $Q_s$ as opposed to a factorization approach done in most saturation and color glass-condensate models, compare [ref] and references within.","intent_p":0.85,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1101.5922","title":"Inclusive hadron distributions in p+p collisions from saturation models of HERA DIS data","url":"/paper/1101.5922","section":"Results and discussion","sentence":"Various kinematic variables exhibit scaling with the saturation scale [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1012.4699","title":"From many body wee parton dynamics to perfect fluid: a standard model for heavy ion collisions","url":"/paper/1012.4699","section":"The little bang and the Glasma","sentence":"These geometrical correlations give rise [ref] to the negative binomial distribution which explains multiplicity distributions [ref] and forward-backward multiplicity correlations [ref] in hadronic collisions.","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":10,"sentences":10,"quotes":[{"arxiv_id":"2203.10296","title":"Soft Pomeron in the Colour Glass Condensate approach","url":"/paper/2203.10296","section":"The master equation","sentence":"We can see that the interaction of the BFKL Pomeron with the proton is known from the DIS data and we have numerous attempts to describe this interaction using the Balitsky-Kovchegov parton cascade [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"2311.06406","title":"CGC and saturation approach: Impact-parameter dependent model of perturbative QCD and combined HERA data","url":"/paper/2311.06406","section":"Introduction","sentence":"In most cases, these models include the non-perturbative $b$-behavior of the scattering amplitude and has been widely applied in what is commonly referred to as saturation models [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"2203.13314","title":"Investigating saturation effects and the virtual pion in leading neutron events at HERA with the dipole model","url":"/paper/2203.13314","section":"Introduction","sentence":"The colour dipole model provides an unified framework to study the inclusive, exclusive, and inclusive diffractive data [ref] gathered in ep collisions and the inclusive particle production data in pp, pA, and AA collisions [ref] at small x.","intent_p":0.95,"contests_p":null},{"arxiv_id":"1508.02544","title":"CGC/saturation approach: a new impact-parameter dependent model","url":"/paper/1508.02544","section":"Introduction.","sentence":"Numerous attempts have been undertaken over the past two decades (see Refs. 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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/1011.1895"}}