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Constraints of the Low-x Structure of Protons and Nuclei

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Figure

Figure 1. Left: Kinematic coverage of DIS data as a function of x and Q2 compared to cut values used in theNNPDF fits
Figure 3. Left: Nuclear modification factorsand nCTEQ15 frameworks. Right: Analytic shape of RPbg of gluon PDFs in Pb at Q2 = 10 GeV2 as obtained in the EPPS16 RAg as used in EPPS16
Figure 4. Nuclear modification factor for D0 production in p–Pb collisions at the LHC as a function of rapidity.Measurements from LHCb and ALICE are compared to refits of nuclear PDF sets nCTEQ15 (left) and EPPS16(right) for one choice of scales
Figure 5. Distributions of x2 probed in forward production at LHC. Left: Distributions for DY pairs and D0mesons in LHCb and for real photons in the proposed forward photon detector (FoCal) in ALICE, from PYTHIA8calculations
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