Comparisons between ALICE $\jpsi$ and $\psi(2S)$ data and summed NRQCD and FONLL model calculations from [35], [36] and [37]. The first five panels correspond to inclusive $\jpsi$ production cross sections as a function of $\pt$ in pp collisions at $\sqrts=13$, $8$, $7$, $5.02$ and $2.76$ TeV (red), the next three panels to inclusive $\psi(2S)$ cross sections as a function of $\pt$ at $\sqrts=13$, $8$ and $7$ TeV (blue) and the last three panels to $\psi(2S)$-to-$\jpsi$ cross section ratios as a function of $\pt$ at the same $\sqrts$ (black). | ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/sigmaJPsiPt_yqma_sum_13TeV_bw-22754.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/sigmaJPsiPt_yqma_sum_8TeV_bw-22755.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/sigmaJPsiPt_yqma_sum_7TeV_bw-22756.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/sigmaJPsiPt_yqma_sum_5TeV_bw-22757.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/sigmaJPsiPt_yqma_sum_3TeV_bw-22758.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/sigmaPsi2SPt_yqma_sum_13TeV_bw-22759.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/sigmaPsi2SPt_yqma_sum_8TeV_bw-22760.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/sigmaPsi2SPt_yqma_sum_7TeV_bw-22761.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/psiRatioPt_yqma_13TeV_bw-22762.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/psiRatioPt_yqma_8TeV_bw-22763.png ) ![](https://alice-publications.web.cern.ch/sites/default/files/papers/3364/psiRatioPt_yqma_7TeV_bw-22764.png ) |