Alfonso Albero, AlejandroCalvo Gomez, M.Camboni, AlessandroCoquereau, SamuelGarrido Beltrán, LluísGascón Fora, DavidGironella Gironell, PereGraciani Díaz, RicardoGraugés Pous, EugeniMarin Benito, CarlaVilasis-Carmona, X.LHCb Collaboration2022-06-132022-06-132019-05-151126-6708https://hdl.handle.net/2445/186557The top plot shown in figure 3 of ref. [1] is the result of 8 TeV. The correct figure is given below in figure 3: (ϒ) [GeV/c] T p 0 5 10 15 )] c [pb/(GeV/ B× T p /d σ d −1 10 10 3 10 LHCb 2.0 < y < 4.5 ϒ (1S) ϒ (2S) ϒ (3S) Figure 3. Differential cross-sections multiplied by dimuon branching fractions for the Υ(1S) (black solid squares), Υ(2S) (red upward triangles) and Υ(3S) (blue downward triangles) states versus pT integrated over y between 2.0 and 4.5. Statistical and systematic uncertainties are added in quadrature. Predictions from NRQCD [2] for the Υ(1S) (black grid shading), Υ(2S) (red grid shading) and Υ(3S) (blue grid shading) states are overlaid in the plot.7 p.application/pdfengcc-by (c) Alfonso Albero, Alejandro et al., 2019https://creativecommons.org/licenses/by/4.0/HadronsGran Col·lisionador d'HadronsFísica de partículesExperimentsHadronsLarge Hadron Collider (France and Switzerland)Particle physicsExperimentsinfo:eu-repo/semantics/article6963422022-06-13info:eu-repo/semantics/openAccess