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Projections of a two-dimensional fit used to extract the prompt \JPsi yield in \PbPb collisions. \cmsLeftI: The dimuon invariant mass distribution. \cmsRightI: The pseudo-proper decay length ($l_{\JPsi}$) distribution. The fit functions are described in the text. The lower panels display the pull distributions, defined as the difference between the fit and the data, divided by the combined statistical uncertainty in the fit and in the data.

Projections of a two-dimensional fit used to extract the prompt \JPsi yield in \PbPb collisions. \cmsLeftI: The dimuon invariant mass distribution. \cmsRightI: The pseudo-proper decay length ($l_{\JPsi}$) distribution. The fit functions are described in the text. The lower panels display the pull distributions, defined as the difference between the fit and the data, divided by the combined statistical uncertainty in the fit and in the data.

Projections of a two-dimensional fit used to extract the prompt \JPsi yield in \PbPb collisions. \cmsLeftI: The dimuon invariant mass distribution. \cmsRightI: The pseudo-proper decay length ($l_{\JPsi}$) distribution. The fit functions are described in the text. The lower panels display the pull distributions, defined as the difference between the fit and the data, divided by the combined statistical uncertainty in the fit and in the data.

Projections of a two-dimensional fit used to extract the prompt \JPsi yield in \PbPb collisions. \cmsLeftI: The dimuon invariant mass distribution. \cmsRightI: The pseudo-proper decay length ($l_{\JPsi}$) distribution. The fit functions are described in the text. The lower panels display the pull distributions, defined as the difference between the fit and the data, divided by the combined statistical uncertainty in the fit and in the data.

Detector response matrices for jets containing a prompt \JPsi meson, showing the bin migration probability as a function of jet \pt and~$z$. The response for $\Pp\Pp$ collisions (\cmsLeft) is evaluated using \PYTHIA 8. The response for \PbPb collisions (\cmsRight) is evaluated using \PYTHIA 8 embedded into \HYDJET.

Detector response matrices for jets containing a prompt \JPsi meson, showing the bin migration probability as a function of jet \pt and~$z$. The response for $\Pp\Pp$ collisions (\cmsLeft) is evaluated using \PYTHIA 8. The response for \PbPb collisions (\cmsRight) is evaluated using \PYTHIA 8 embedded into \HYDJET.

Detector response matrices for jets containing a prompt \JPsi meson, showing the bin migration probability as a function of jet \pt and~$z$. The response for $\Pp\Pp$ collisions (\cmsLeft) is evaluated using \PYTHIA 8. The response for \PbPb collisions (\cmsRight) is evaluated using \PYTHIA 8 embedded into \HYDJET.

Detector response matrices for jets containing a prompt \JPsi meson, showing the bin migration probability as a function of jet \pt and~$z$. The response for $\Pp\Pp$ collisions (\cmsLeft) is evaluated using \PYTHIA 8. The response for \PbPb collisions (\cmsRight) is evaluated using \PYTHIA 8 embedded into \HYDJET.

The main sources of systematic uncertainty, as a function of $z$, for the cross section in $\Pp\Pp$ (\cmsLeft) and the $T_{\tAA}$-scaled yield in \PbPb (\cmsRight) collisions. The normalization uncertainties of 1.9\% for $\Pp\Pp$ and 2.6\% for \PbPb are not shown.

The main sources of systematic uncertainty, as a function of $z$, for the cross section in $\Pp\Pp$ (\cmsLeft) and the $T_{\tAA}$-scaled yield in \PbPb (\cmsRight) collisions. The normalization uncertainties of 1.9\% for $\Pp\Pp$ and 2.6\% for \PbPb are not shown.

The main sources of systematic uncertainty, as a function of $z$, for the cross section in $\Pp\Pp$ (\cmsLeft) and the $T_{\tAA}$-scaled yield in \PbPb (\cmsRight) collisions. The normalization uncertainties of 1.9\% for $\Pp\Pp$ and 2.6\% for \PbPb are not shown.

The main sources of systematic uncertainty, as a function of $z$, for the cross section in $\Pp\Pp$ (\cmsLeft) and the $T_{\tAA}$-scaled yield in \PbPb (\cmsRight) collisions. The normalization uncertainties of 1.9\% for $\Pp\Pp$ and 2.6\% for \PbPb are not shown.

Normalized $z$ distribution in $\Pp\Pp$ collisions, compared to prompt and nonprompt \JPsi in \PYTHIA 8, at the generator level. Bars indicate statistical uncertainties, while systematic uncertainties are depicted as boxes.

Normalized $z$ distribution in $\Pp\Pp$ collisions, compared to prompt and nonprompt \JPsi in \PYTHIA 8, at the generator level. Bars indicate statistical uncertainties, while systematic uncertainties are depicted as boxes.

\cmsLeftI: The \JPsi differential cross section in $\Pp\Pp$ and the $T_{\tAA}$-scaled yield in \PbPb collisions, as a function of $z$. The normalization uncertainties of 1.9\% for $\Pp\Pp$ and 2.6\% for \PbPb are not included in the point-by-point uncertainty boxes and not shown in the plot. \cmsRightI: The nuclear modification factor \RAA, as a function of $z$. Bars indicate statistical uncertainties, while systematic uncertainties are depicted as boxes. The box around unity shows the normalization uncertainty.

\cmsLeftI: The \JPsi differential cross section in $\Pp\Pp$ and the $T_{\tAA}$-scaled yield in \PbPb collisions, as a function of $z$. The normalization uncertainties of 1.9\% for $\Pp\Pp$ and 2.6\% for \PbPb are not included in the point-by-point uncertainty boxes and not shown in the plot. \cmsRightI: The nuclear modification factor \RAA, as a function of $z$. Bars indicate statistical uncertainties, while systematic uncertainties are depicted as boxes. The box around unity shows the normalization uncertainty.

\cmsLeftI: The \JPsi differential cross section in $\Pp\Pp$ and the $T_{\tAA}$-scaled yield in \PbPb collisions, as a function of $z$. The normalization uncertainties of 1.9\% for $\Pp\Pp$ and 2.6\% for \PbPb are not included in the point-by-point uncertainty boxes and not shown in the plot. \cmsRightI: The nuclear modification factor \RAA, as a function of $z$. Bars indicate statistical uncertainties, while systematic uncertainties are depicted as boxes. The box around unity shows the normalization uncertainty.

\cmsLeftI: The \JPsi differential cross section in $\Pp\Pp$ and the $T_{\tAA}$-scaled yield in \PbPb collisions, as a function of $z$. The normalization uncertainties of 1.9\% for $\Pp\Pp$ and 2.6\% for \PbPb are not included in the point-by-point uncertainty boxes and not shown in the plot. \cmsRightI: The nuclear modification factor \RAA, as a function of $z$. Bars indicate statistical uncertainties, while systematic uncertainties are depicted as boxes. The box around unity shows the normalization uncertainty.

The nuclear modification factor \RAA for two centrality selections of \PbPb collisions, as a function of $z$. Due to limited statistical precision, the lowest $z$ bin is excluded. Bars indicate statistical uncertainties, while systematic uncertainties are depicted as boxes. The boxes around unity show the normalization uncertainties.

The nuclear modification factor \RAA for two centrality selections of \PbPb collisions, as a function of $z$. Due to limited statistical precision, the lowest $z$ bin is excluded. Bars indicate statistical uncertainties, while systematic uncertainties are depicted as boxes. The boxes around unity show the normalization uncertainties.