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Mid-rapidity prompt quarkonium cross sections measured in pp collisions at $\sqrt{s} = 7$\,TeV by ATLAS (red markers)~\cite{bib:ATLASpsi2S, bib:ATLASchic} and CMS (blue markers)~\cite{bib:BPH-14-001}. The inset shows the \ChicTwo to \ChicOne cross section ratio~\cite{bib:BPH-11-010}. The curves represent the result of the fit described in the text.
: Polar anisotropy parameter \lth, in the helicity frame, measured by CMS in pp collisions at $\sqrt{s} = 7$\,TeV, for prompt \jpsi and \psip dimuon decays~\cite{bib:BPH-13-003}. Values corresponding to two (\jpsi) or three (\psip) rapidity bins were averaged. The curves represent the result of the fit described in the text.
: The $\ChicTwo / \ChicOne$ yield ratio vs.\ \abscosth (in the helicity frame), for three \jpsi \pt bins (8--12, 12--18 and 18--30\,GeV), as measured by CMS in pp collisions at $\sqrt{s} = 8$\,TeV~\cite{bib:BPH-13-001}. The curves represent the result of the fit described in the text.
The fractions of the total prompt \jpsi production rate due to feed-down decays from the \ChicOne, \ChicTwo and \psip mesons, as a function of \pTovM.
The polarization parameter \lth of the \ChicOne and \ChicTwo mesons (left), as well as of the \jpsi mesons directly produced (same as of the \psip) and produced in \ChicOne plus \ChicTwo decays (right), as a function of \pTovM.
: Ratio between the \ChicTwo and \ChicOne cross sections, times the corresponding $\ChicJ \to \jpsi \, \gamma$ branching fractions, as a function of \pTovM, for two extreme polarization scenarios (left) and for the polarizations determined in our global-fit analysis (right).
: Two-dimensional distributions showing the correlations between the \lthTwo and \lthOne polarizations (left) and between the \ChicTwo and \ChicOne feed-down contributions to the prompt \jpsi production rate (right). The results of the three fit variants are represented by the solid ($4\beta$), dashed ($1\beta$) and dotted-dashed ($6\beta$) lines.
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Two-dimensional distributions showing the correlations between the \lth polarization parameters of the \ChicOne or \ChicTwo mesons and the corresponding values for the \jpsi (left), the \psip (middle) and the difference between the two (right). The results of the three fit variants are represented by the solid ($4\beta$), dashed ($1\beta$) and dotted-dashed ($6\beta$) lines.
Two-dimensional distributions showing the correlation between the \lthOne (\lthTwo) observable and the \ChicOne (\ChicTwo) feed-down contribution to the prompt \jpsi production rate. The results of the three fit variants are represented by the solid ($4\beta$), dashed ($1\beta$) and dotted-dashed ($6\beta$) lines.
Two-dimensional distributions showing the correlation between the \lthTwo and \lthOne polarizations, in the $1\beta$ fit variant, when using three sets of measurements: only the direct \ChicJ polarization data~\cite{bib:BPH-13-001} (blue), which essentially constrains the $\lthTwo - \lthOne$ difference, all the other data (red), mostly constraining the $\lthOne + \lthTwo$ sum, and the result of the global fit presented in this paper (pink).