Measurement of the $J/\psi$ and $\psi(2S)$ cross section in pp collisions at √s = 7 TeV

Abstract

A measurement of the J/ψ and ψ(2S) meson production cross sections in pp collisions at data at √s = 7 TeV with the CMS experiment at the LHC. The data correspond to an integrated luminosity of 36.7 pb−1. The two cross sections and their ratio have been measured as a function of the meson transverse momentum pT (up to 70 GeV/c for the J/ψ and to 30 GeV/c for the ψ(2S)) in several rapidity ranges, assuming null polarization in the prompt production. The b-hadron component is then determined from a fit to the decay length distribution. The differential cross- section ratio between the two states is also computed, cancelling out many systematic uncertainties.

Approved plots and figures ( click on plot to download the PDF )

Figure Caption
ALLmassfitJpsi_pT12-15_y09-12.pdf J/ψ mass distribution fit in the bin: 0.9 < abs(y) < 1.2, 12.0 < pT < 15.0 GeV/c.
ALLmassfitPsip_pT8-9_y0-12.pdf J/ψ and ψ(2S) mass distribution fit in the bin: abs(y) < 1.2, 8.0 < pT < 9.0 GeV/c.
XS_all_alsoOld_sg_jpsi.pdf Measured differential cross section for J/ψ inclusive production as a function of pT for five rapidity bins, plotted with the results published in [4], which extend to a lower pT range. (Multiplicative factors - showing as additive offsets in log scale - are used to achieve a convenient graphical separation of the measurements from different rapidity bins.)
2D_ALLtimefitJpsi_pT8-9_y0-09_Log.pdf Projection of a J/ψ two-dimensional fit on the J/ψ decay length dimension in the bin: abs(y) < 0.9, 8.0 < pT < 9.0 GeV/c. The plot below show the distribution of the pulls.
2D_ALLtimefitPsip_pT12-15_y16-24_Log.pdf Projection of a J/ψ-ψ(2S) two-dimensional fit on the ψ(2S) decay length dimension in the bin: 1.6 < abs(y) < 2.4, 12.0 < pT < 15.0 GeV/c. The plots below the distributions show the fit pulls.
XS_all_p_sg_jpsi_teor.pdf Measured differential cross section for prompt J/ψ production as a function of pT for the different rapidity bins. The yellow and blue coloured histograms indicate the theoretical predictions from NRQCD calculations, the lines are added only for illustrative purposes.
XS_all_p_sg_psi2s_teor.pdf Measured differential cross section for prompt ψ(2S) production as a function of pT for the different rapidity bins. The yellow and blue coloured histograms indicate the theoretical predictions from NRQCD calculations, the lines are added only for illustrative purposes.
XS_all_b_sg_jpsi_teor.pdf Measured differential cross section for non-prompt J/ψ production as a function of pT for the different rapidity bins. The yellow and blue coloured histograms indicate the theoretical predictions from FONLL calculations, the lines are added only for illustrative purposes.
XS_all_b_sg_psi2s_teor.pdf Measured differential cross section for non-prompt ψ(2S) production as a function of pT for the different rapidity bins. The yellow and blue coloured histograms indicate the theoretical predictions from FONLL calculations, the lines are added only for illustrative purposes
XS_all_p_sg_noAcc_jpsi.pdf Measured differential cross section for prompt J/psi production as a function of pT for the different rapidity bins. The error bars on data points include all the statistical and systematic contributions except luminosity. The measurements have been offset by the numerical values given in the legend for easier viewing. The results are not corrected for the muon acceptance
XS_all_p_sg_noAcc_psi2s.pdf Measured differential cross section for prompt psi(2S) production as a function of pT for the different rapidity bins. The error bars on data points include all the statistical and systematic contributions except luminosity. The measurements have been offset by the numerical values given in the legend for easier viewing. The results are not corrected for the muon acceptance.
XS_all_b_sg_noAcc_jpsi.pdf Measured differential cross section for non-prompt J/psi production as a function of pT for the different rapidity bins. The error bars on data points include all the statistical and systematic contributions except luminosity. The measurements have been offset by the numerical values given in the legend for easier viewing. The result is not corrected for the muon acceptance.
XS_all_b_sg_noAcc_psi2s.pdf Measured differential cross section for non-prompt psi(2S) production as a function of pT for the different rapidity bins. The error bars on data points include all the statistical and systematic contributions except luminosity. The measurements have been offset by the numerical values given in the legend for easier viewing. The result is not corrected for the muon acceptance.
bfrac_0-12.pdf Fitted J/ψ and ψ(2S) b-fractions plotted as a function of pT for abs(y) < 1.2.
bfrac_12-16.pdf Fitted J/ψ and ψ(2S) b-fractions plotted as a function of pT for 1.2 < abs(y) < 1.6.
bfrac_16-24.pdf Fitted J/ψ and ψ(2S) b-fractions plotted as a function of pT for 1.6 < abs(y) < 2.4.
PRatio_av.pdf Measured value of the &psi(2S) to J/&psi differential cross-section ratio, for prompt production, averaged over rapidity and plotted as a function of pT. It also includes the comparison with the NRQCD prediction. The shaded bands show the uncertainties on the theoretical predictions. The error bars give the total uncertainties on the measurements; polarization uncertainties are not included.
BRatio_av.pdf Measured value of the &psi(2S) to J/&psi differential cross-section ratio, for non-prompt production, averaged over rapidity and plotted as a function of pT. It also shows the predictions of the theoretical models used to determine BR(B -> &psi(2S) X), after the latter have been rescaled to the fitted value given in Eq. (12). The shaded bands show the uncertainties on the theoretical predictions. The error bars give the total uncertainties on the measurements.

Tables of numerical results

Cross Sections

All results are expressed in nb / (GeV/c).

Absolute J/psi cross section (divided by unpolarized acceptance)

Prompt
 \begin{table}[htdp] \begin{tabular}{lccccc} \hline $p_T$ (GeV/c)   &amp;   $<p_T>$ (GeV/c)   &amp;  $\frac{d^2\sigma}{dp_\mathrm{T}dy} \cdot  \mbox{BR} \cdot (1-f_b)$   &amp;   $\pm \sigma_{\mathrm{stat}} $   &amp;   $\pm \sigma_{\mathrm{syst}} $ &amp; $\pm \sigma_{\mathrm{lumi}}$ \\ \hline \multicolumn{6}{c}{$0 < |y| < 0.9 $} \\ \hline $8.0-9.0$   &amp; $8.569 \pm 0.003$ &amp;  $2.54 $ &amp; $ 0.07 $ &amp; $ 0.06 $ &amp; $ 0.10$ \\ $9.0-10.0$  &amp; $9.515 \pm 0.002$ &amp;  $1.56 $ &amp; $ 0.03 $ &amp; $ 0.09 $ &amp; $ 0.06$ \\ $10.0-11.0$ &amp; $10.494 \pm 0.002$ &amp; $0.96 $ &amp; $ 0.02 $ &amp; $ 0.04 $ &amp; $ 0.04$ \\ $11.0-12.0$ &amp; $11.485 \pm 0.002$ &amp; $0.612 $ &amp; $ 0.012 $ &amp; $ 0.025 $ &amp; $ 0.024$ \\ $12.0-13.5$ &amp; $12.711 \pm 0.003$ &amp; $0.351 $ &amp; $ 0.006 $ &amp; $ 0.013 $ &amp; $ 0.014$ \\ $13.5-15.0$ &amp; $14.206 \pm 0.004$ &amp; $0.184 $ &amp; $ 0.004 $ &amp; $ 0.005 $ &amp; $ 0.007$ \\ $15.0-18.0$ &amp; $16.329 \pm 0.007$ &amp; $0.0841 $ &amp; $ 0.0015 $ &amp; $ 0.0024 $ &amp; $ 0.0034$ \\ $18.0-30.0$ &amp; $21.77 \pm 0.02$ &amp;   $0.0139 $ &amp; $ 0.0002 $ &amp; $ 0.0005 $ &amp; $ 0.0006$ \\ $30.0-45.0$ &amp; $35.03 \pm 0.08$ &amp;   $0.00078 $ &amp; $ 0.00003 $ &amp; $ 0.00003 $ &amp; $ 0.00003$ \\ $45.0-70.0$ &amp; $52.7 \pm 0.3$ &amp;     $0.000070 $ &amp; $ 0.000007 $ &amp; $ 0.000017 $ &amp; $ 0.000003$ \\ \hline	      			    \multicolumn{6}{c}{$0.9 < |y| < 1.2 $} \\ \hline	      			    $8.0-9.0$   &amp; $8.524 \pm 0.002$ &amp;  $2.62 $ &amp; $ 0.08 $ &amp; $ 0.15 $ &amp; $ 0.10$ \\ $9.0-10.0$  &amp; $9.491 \pm 0.003$ &amp;  $1.55 $ &amp; $ 0.05 $ &amp; $ 0.12 $ &amp; $ 0.06$ \\ $10.0-12.0$ &amp; $10.921 \pm 0.004$ &amp; $0.75 $ &amp; $ 0.02 $ &amp; $ 0.04 $ &amp; $ 0.03$ \\ $12.0-15.0$ &amp; $13.312 \pm 0.008$ &amp; $0.248 $ &amp; $ 0.006 $ &amp; $ 0.013 $ &amp; $ 0.010$ \\ $15.0-30.0$ &amp; $18.95 \pm 0.03$ &amp;   $0.0264 $ &amp; $ 0.0006 $ &amp; $ 0.0007 $ &amp; $ 0.0011$ \\ $30.0-45.0$ &amp; $34.7 \pm 0.1$ &amp;   $0.00067 $ &amp; $ 0.00006 $ &amp; $ 0.00005 $ &amp; $ 0.00003$ \\ \hline	      		       	    \multicolumn{6}{c}{$1.2 < |y| < 1.6 $} \\ \hline	      			    $6.5-7.0$   &amp;  $6.771 \pm 0.002$ &amp; $7.09 $ &amp; $ 0.44 $ &amp; $ 0.30 $ &amp; $ 0.28$ \\ $7.0-7.5$   &amp; $7.268 \pm 0.002$ &amp; $5.28 $ &amp; $ 0.24 $ &amp; $ 0.11 $ &amp; $ 0.21$ \\ $7.5-8.0$   &amp; $7.756 \pm 0.001$ &amp; $4.16 $ &amp; $ 0.16 $ &amp; $ 0.12 $ &amp; $ 0.17$ \\ $8.0-8.5$   &amp; $8.255 \pm 0.001$ &amp; $2.92 $ &amp; $ 0.10 $ &amp; $ 0.10 $ &amp; $ 0.12$ \\ $8.5-9.0$   &amp; $8.748 \pm 0.001$ &amp; $2.24 $ &amp; $ 0.08 $ &amp; $ 0.13 $ &amp; $ 0.09$ \\ $9.0-10.0$  &amp; $9.486 \pm 0.002$ &amp; $1.47 $ &amp; $ 0.04 $ &amp; $ 0.06 $ &amp; $ 0.06$ \\ $10.0-11.0$ &amp; $10.478 \pm 0.002$ &amp; $0.84 $ &amp; $ 0.02 $ &amp; $ 0.03 $ &amp; $ 0.03$ \\ $11.0-12.0$ &amp; $11.475 \pm 0.003$ &amp; $0.528 $ &amp; $ 0.015 $ &amp; $ 0.020 $ &amp; $ 0.021$ \\ $12.0-15.0$ &amp; $13.293 \pm 0.007$ &amp; $0.227 $ &amp; $ 0.005 $ &amp; $ 0.008 $ &amp; $ 0.009$ \\ $15.0-30.0$ &amp; $18.84 \pm 0.03$ &amp; $0.0232 $ &amp; $ 0.0005 $ &amp; $ 0.0007 $ &amp; $ 0.0009$ \\ $30.0-45.0$ &amp; $34.9 \pm 0.1$ &amp; $0.00080 $ &amp; $ 0.00008 $ &amp; $ 0.00006 $ &amp; $ 0.00003$ \\ \hline	      			    \multicolumn{6}{c}{$1.6 < |y| < 2.1 $} \\ \hline	      	   		    $6.5-7.0$   &amp; $6.776 \pm 0.002$ &amp; $7.7 $ &amp; $ 0.4 $ &amp; $ 0.4 $ &amp; $ 0.3$ \\ $7.0-7.25$  &amp; $7.129 \pm 0.001$ &amp; $5.73 $ &amp; $ 0.34 $ &amp; $ 0.30 $ &amp; $ 0.23$ \\ $7.25-7.5$  &amp; $7.374 \pm 0.001$ &amp; $5.04 $ &amp; $ 0.29 $ &amp; $ 0.27 $ &amp; $ 0.20$ \\ $7.5-8.0$   &amp; $7.752 \pm 0.001$ &amp; $3.76 $ &amp; $ 0.16 $ &amp; $ 0.22 $ &amp; $ 0.15$ \\ $8.0-8.5$   &amp; $8.247 \pm 0.002$ &amp; $2.67 $ &amp; $ 0.11 $ &amp; $ 0.13 $ &amp; $ 0.11$ \\ $8.5-9.0$   &amp; $8.745 \pm 0.002$ &amp; $2.18 $ &amp; $ 0.09 $ &amp; $ 0.09 $ &amp; $ 0.09$ \\ $9.0-10.0$  &amp; $9.474 \pm 0.003$ &amp; $1.50 $ &amp; $ 0.04 $ &amp; $ 0.06 $ &amp; $ 0.06$ \\ $10.0-11.0$ &amp; $10.474 \pm 0.003$ &amp; $0.84 $ &amp; $ 0.03 $ &amp; $ 0.04 $ &amp; $ 0.03$ \\ $11.0-12.0$ &amp; $11.475 \pm 0.003$ &amp; $0.512 $ &amp; $ 0.018 $ &amp; $ 0.025 $ &amp; $ 0.020$ \\ $12.0-15.0$ &amp; $13.273 \pm 0.008$ &amp; $0.232 $ &amp; $ 0.006 $ &amp; $ 0.011 $ &amp; $ 0.009$ \\ $15.0-30.0$ &amp; $18.71 \pm 0.04$ &amp; $0.0220 $ &amp; $ 0.0006 $ &amp; $ 0.0009 $ &amp; $ 0.0009$ \\ \hline	      			    \multicolumn{6}{c}{$2.1 < |y| < 2.4 $} \\ \hline	      			    $5.5-8.0$   &amp; $7.153 \pm 0.008$ &amp;  $5.26 $ &amp; $ 0.31 $ &amp; $ 0.28 $ &amp; $ 0.21$ \\ $8.0-9.0$   &amp; $8.490 \pm 0.006$ &amp;  $2.52 $ &amp; $ 0.20 $ &amp; $ 0.16 $ &amp; $ 0.10$ \\ $9.0-10.0$  &amp; $9.488 \pm 0.006$ &amp; $1.30 $ &amp; $ 0.10 $ &amp; $ 0.11 $ &amp; $ 0.05$ \\ $10.0-12.0$ &amp; $10.91 \pm 0.01$ &amp; $0.66 $ &amp; $ 0.04 $ &amp; $ 0.07 $ &amp; $ 0.03$ \\ $12.0-15.0$ &amp; $13.29 \pm 0.01$ &amp; $0.207 $ &amp; $ 0.011 $ &amp; $ 0.017 $ &amp; $ 0.008$ \\ $15.0-30.0$ &amp; $18.57 \pm 0.08$ &amp; $0.0171 $ &amp; $ 0.0010 $ &amp; $ 0.0013 $ &amp; $ 0.0007$ \\ \hline \end{tabular} \end{table}

Non Prompt
 \begin{table}[htdp] \begin{tabular}{lcccc} \hline $p_T$ (GeV/c)   &amp;   $\frac{d^2\sigma}{dp_\mathrm{T}dy} \cdot  \mbox{BR} \cdot f_b$   &amp;   $\pm \sigma_{\mathrm{stat}} $   &amp;   $\pm \sigma_{\mathrm{syst}} $ &amp; $\pm \sigma_{\mathrm{lumi}}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 0.9 $} \\ \hline $8.0-9.0$ &amp; $0.946 $ &amp; $ 0.025 $ &amp; $ 0.025 $ &amp; $ 0.038$ \\ $9.0-10.0$ &amp; $0.62 $ &amp; $ 0.01 $ &amp; $ 0.04 $ &amp; $ 0.02$ \\ $10.0-11.0$ &amp; $0.451 $ &amp; $ 0.009 $ &amp; $ 0.021 $ &amp; $ 0.018$ \\ $11.0-12.0$ &amp; $0.322 $ &amp; $ 0.006 $ &amp; $ 0.014 $ &amp; $ 0.013$ \\ $12.0-13.5$ &amp; $0.209 $ &amp; $ 0.004 $ &amp; $ 0.008 $ &amp; $ 0.008$ \\ $13.5-15.0$ &amp; $0.131 $ &amp; $ 0.003 $ &amp; $ 0.004 $ &amp; $ 0.005$ \\ $15.0-18.0$ &amp; $0.0700 $ &amp; $ 0.0013 $ &amp; $ 0.0020 $ &amp; $ 0.0028$ \\ $18.0-30.0$ &amp; $0.0160 $ &amp; $ 0.0003 $ &amp; $ 0.0006 $ &amp; $ 0.0006$ \\ $30.0-45.0$ &amp; $0.00134 $ &amp; $ 0.00006 $ &amp; $ 0.00005 $ &amp; $ 0.00005$ \\ $45.0-70.0$ &amp; $0.00013 $ &amp; $ 0.00001 $ &amp; $ 0.00003 $ &amp; $ 0.00001$ \\ \hline \multicolumn{5}{c}{$0.9 < |y| < 1.2 $} \\ \hline $8.0-9.0$ &amp; $0.94 $ &amp; $ 0.03 $ &amp; $ 0.06 $ &amp; $ 0.04$ \\ $9.0-10.0$ &amp; $0.60 $ &amp; $ 0.02 $ &amp; $ 0.05 $ &amp; $ 0.02$ \\ $10.0-12.0$ &amp; $0.358 $ &amp; $ 0.008 $ &amp; $ 0.020 $ &amp; $ 0.014$ \\ $12.0-15.0$ &amp; $0.152 $ &amp; $ 0.004 $ &amp; $ 0.008 $ &amp; $ 0.006$ \\ $15.0-30.0$ &amp; $0.0245 $ &amp; $ 0.0006 $ &amp; $ 0.0006 $ &amp; $ 0.0010$ \\ $30.0-45.0$ &amp; $0.00107 $ &amp; $ 0.00009 $ &amp; $ 0.00006 $ &amp; $ 0.00004$ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $6.5-7.0$ &amp; $1.85 $ &amp; $ 0.12 $ &amp; $ 0.09 $ &amp; $ 0.07$ \\ $7.0-7.5$ &amp; $1.50 $ &amp; $ 0.07 $ &amp; $ 0.05 $ &amp; $ 0.06$ \\ $7.5-8.0$ &amp; $1.17 $ &amp; $ 0.04 $ &amp; $ 0.07 $ &amp; $ 0.05$ \\ $8.0-8.5$ &amp; $0.91 $ &amp; $ 0.03 $ &amp; $ 0.05 $ &amp; $ 0.04$ \\ $8.5-9.0$ &amp; $0.76 $ &amp; $ 0.03 $ &amp; $ 0.05 $ &amp; $ 0.03$ \\ $9.0-10.0$ &amp; $0.558 $ &amp; $ 0.014 $ &amp; $ 0.027 $ &amp; $ 0.022$ \\ $10.0-11.0$ &amp; $0.357 $ &amp; $ 0.010 $ &amp; $ 0.017 $ &amp; $ 0.014$ \\ $11.0-12.0$ &amp; $0.267 $ &amp; $ 0.008 $ &amp; $ 0.012 $ &amp; $ 0.011$ \\ $12.0-15.0$ &amp; $0.137 $ &amp; $ 0.003 $ &amp; $ 0.006 $ &amp; $ 0.005$ \\ $15.0-30.0$ &amp; $0.0202 $ &amp; $ 0.0004 $ &amp; $ 0.0007 $ &amp; $ 0.0008$ \\ $30.0-45.0$ &amp; $0.00113 $ &amp; $ 0.00011 $ &amp; $ 0.00006 $ &amp; $ 0.00005$ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.1 $} \\ \hline $6.5-7.0$ &amp; $1.92 $ &amp; $ 0.10 $ &amp; $ 0.16 $ &amp; $ 0.08$ \\ $7.0-7.25$ &amp; $1.67 $ &amp; $ 0.10 $ &amp; $ 0.11 $ &amp; $ 0.07$ \\ $7.25-7.5$ &amp; $1.59 $ &amp; $ 0.09 $ &amp; $ 0.10 $ &amp; $ 0.06$ \\ $7.5-8.0$ &amp; $1.14 $ &amp; $ 0.05 $ &amp; $ 0.09 $ &amp; $ 0.05$ \\ $8.0-8.5$ &amp; $0.83 $ &amp; $ 0.03 $ &amp; $ 0.06 $ &amp; $ 0.03$ \\ $8.5-9.0$ &amp; $0.73 $ &amp; $ 0.03 $ &amp; $ 0.05 $ &amp; $ 0.03$ \\ $9.0-10.0$ &amp; $0.52 $ &amp; $ 0.02 $ &amp; $ 0.03 $ &amp; $ 0.02$ \\ $10.0-11.0$ &amp; $0.357 $ &amp; $ 0.011 $ &amp; $ 0.019 $ &amp; $ 0.014$ \\ $11.0-12.0$ &amp; $0.242 $ &amp; $ 0.008 $ &amp; $ 0.016 $ &amp; $ 0.010$ \\ $12.0-15.0$ &amp; $0.128 $ &amp; $ 0.003 $ &amp; $ 0.008 $ &amp; $ 0.005$ \\ $15.0-30.0$ &amp; $0.0186 $ &amp; $ 0.0005 $ &amp; $ 0.0009 $ &amp; $ 0.0007$ \\ \hline \multicolumn{5}{c}{$2.1 < |y| < 2.4 $} \\ \hline $5.5-8.0$ &amp; $1.43 $ &amp; $ 0.08 $ &amp; $ 0.11 $ &amp; $ 0.06$ \\ $8.0-9.0$ &amp; $0.74 $ &amp; $ 0.06 $ &amp; $ 0.08 $ &amp; $ 0.03$ \\ $9.0-10.0$ &amp; $0.49 $ &amp; $ 0.04 $ &amp; $ 0.05 $ &amp; $ 0.02$ \\ $10.0-12.0$ &amp; $0.27 $ &amp; $ 0.02 $ &amp; $ 0.03 $ &amp; $ 0.01$ \\ $12.0-15.0$ &amp; $0.121 $ &amp; $ 0.006 $ &amp; $ 0.011 $ &amp; $ 0.005$ \\ $15.0-30.0$ &amp; $0.0131 $ &amp; $ 0.0008 $ &amp; $ 0.0011 $ &amp; $ 0.0005$ \\ \hline \end{tabular} \end{table}

Absolute psi(2S) cross section (divided by unpolarized acceptance)

Prompt
 \begin{table}[htdp] \begin{tabular}{lccccc} \hline $p_T$ (GeV/c)   &amp;  $<p_T>$ (GeV/c)   &amp;   $\frac{d^2\sigma}{dp_\mathrm{T}dy} \cdot  \mbox{BR} \cdot (1-f_b)$   &amp;   $\pm \sigma_{\mathrm{stat}} $   &amp;   $\pm \sigma_{\mathrm{syst}} $ &amp; $\pm \sigma_{\mathrm{lumi}}$ \\ \hline \multicolumn{6}{c}{$0 < |y| < 1.2 $} \\ \hline $6.5-8.0$  &amp; $7.60 \pm 0.02$   &amp; $0.148 $ &amp; $ 0.029 $ &amp; $ 0.020 $ &amp; $ 0.006$ \\ $8.0-9.0$  &amp; $8.54 \pm 0.02$   &amp; $0.083 $ &amp; $ 0.008 $ &amp; $ 0.006 $ &amp; $ 0.003$ \\ $9.0-10.0$ &amp; $9.50 \pm 0.02$   &amp; $0.061 $ &amp; $ 0.005 $ &amp; $ 0.004 $ &amp; $ 0.002$ \\ $10.0-11.0$ &amp; $10.50 \pm 0.02$  &amp; $0.0368 $ &amp; $ 0.0031 $ &amp; $ 0.0023 $ &amp; $ 0.0015$ \\ $11.0-12.0$ &amp; $11.48 \pm 0.02$  &amp; $0.0217 $ &amp; $ 0.0019 $ &amp; $ 0.0022 $ &amp; $ 0.0009$ \\ $12.0-13.5$ &amp; $12.72 \pm 0.02$  &amp; $0.0141 $ &amp; $ 0.0011 $ &amp; $ 0.0010 $ &amp; $ 0.0006$ \\ $13.5-15.0$ &amp; $14.23 \pm 0.03$  &amp; $0.0077 $ &amp; $ 0.0007 $ &amp; $ 0.0006 $ &amp; $ 0.0003$ \\ $15.0-18.0$ &amp; $16.30 \pm 0.05$  &amp; $0.00368 $ &amp; $ 0.00030 $ &amp; $ 0.00017 $ &amp; $ 0.00015$ \\ $18.0-30.0$ &amp; $21.92 \pm 0.18$  &amp; $0.00066 $ &amp; $ 0.00005 $ &amp; $ 0.00005 $ &amp; $ 0.00003$ \\ \hline	   		        \multicolumn{6}{c}{$1.2 < |y| < 1.6 $} \\ \hline	   		        $5.5-6.5$  &amp; $6.15 \pm 0.04$   &amp; $0.62 $ &amp; $ 0.31 $ &amp; $ 0.05 $ &amp; $ 0.02$ \\ $6.5-8.0$  &amp; $7.36 \pm 0.03$   &amp; $0.187 $ &amp; $ 0.023 $ &amp; $ 0.005 $ &amp; $ 0.007$ \\ $8.0-9.0$  &amp; $8.49 \pm 0.02$   &amp; $0.078 $ &amp; $ 0.011 $ &amp; $ 0.005 $ &amp; $ 0.003$ \\ $9.0-10.0$ &amp; $9.50 \pm 0.02$   &amp; $0.058 $ &amp; $ 0.009 $ &amp; $ 0.006 $ &amp; $ 0.002$ \\ $10.0-12.0$ &amp; $10.97 \pm 0.03$  &amp; $0.0264 $ &amp; $ 0.0031 $ &amp; $ 0.0020 $ &amp; $ 0.0011$ \\ $12.0-15.0$ &amp; $13.32 \pm 0.06$  &amp; $0.0109 $ &amp; $ 0.0013 $ &amp; $ 0.0014 $ &amp; $ 0.0004$ \\ $15.0-30.0$ &amp; $19.07 \pm 0.23$  &amp; $0.00132 $ &amp; $ 0.00013 $ &amp; $ 0.00011 $ &amp; $ 0.00005$ \\ \hline	   		        \multicolumn{6}{c}{$1.6 < |y| < 2.4 $} \\ \hline	   		        $5.5-6.5$  &amp; $6.20 \pm 0.02$   &amp; $0.43 $ &amp; $ 0.15 $ &amp; $ 0.13 $ &amp; $ 0.02$ \\ $6.5-8.0$  &amp; $7.25 \pm 0.02$   &amp; $0.185 $ &amp; $ 0.031 $ &amp; $ 0.014 $ &amp; $ 0.007$ \\ $8.0-9.0$  &amp;  $8.48 \pm 0.02$  &amp; $0.078 $ &amp; $ 0.011 $ &amp; $ 0.008 $ &amp; $ 0.003$ \\ $9.0-10.0$ &amp;  $9.52 \pm 0.02$  &amp; $0.049 $ &amp; $ 0.008 $ &amp; $ 0.007 $ &amp; $ 0.002$ \\ $10.0-12.0$ &amp; $10.88 \pm 0.03$  &amp; $0.0219 $ &amp; $ 0.0028 $ &amp; $ 0.0026 $ &amp; $ 0.0009$ \\ $12.0-15.0$ &amp; $13.38 \pm 0.05$  &amp; $0.0090 $ &amp; $ 0.0011 $ &amp; $ 0.0008 $ &amp; $ 0.0004$ \\ $15.0-30.0$ &amp; $19.01 \pm 0.23$  &amp; $0.00093 $ &amp; $ 0.00012 $ &amp; $ 0.00008 $ &amp; $ 0.00004$ \\ \hline \end{tabular} \end{table}

Non Prompt
 \begin{table}[htdp] \begin{tabular}{lcccc} \hline $p_T$ (GeV/c)   &amp;   $\frac{d^2\sigma}{dp_\mathrm{T}dy} \cdot  \mbox{BR} \cdot f_b$   &amp;   $\pm \sigma_{\mathrm{stat}} $   &amp;   $\pm \sigma_{\mathrm{syst}} $ &amp; $\pm \sigma_{\mathrm{lumi}}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 1.2 $} \\ \hline $6.5-8.0$ &amp; $0.072 $ &amp; $ 0.014 $ &amp; $ 0.010 $ &amp; $ 0.003$ \\ $8.0-9.0$ &amp; $0.045 $ &amp; $ 0.004 $ &amp; $ 0.003 $ &amp; $ 0.002$ \\ $9.0-10.0$ &amp; $0.0307 $ &amp; $ 0.0026 $ &amp; $ 0.0026 $ &amp; $ 0.0012$ \\ $10.0-11.0$ &amp; $0.0223 $ &amp; $ 0.0019 $ &amp; $ 0.0017 $ &amp; $ 0.0009$ \\ $11.0-12.0$ &amp; $0.0142 $ &amp; $ 0.0013 $ &amp; $ 0.0017 $ &amp; $ 0.0006$ \\ $12.0-13.5$ &amp; $0.0107 $ &amp; $ 0.0008 $ &amp; $ 0.0008 $ &amp; $ 0.0004$ \\ $13.5-15.0$ &amp; $0.0065 $ &amp; $ 0.0006 $ &amp; $ 0.0006 $ &amp; $ 0.0003$ \\ $15.0-18.0$ &amp; $0.00350 $ &amp; $ 0.00028 $ &amp; $ 0.00016 $ &amp; $ 0.00014$ \\ $18.0-30.0$ &amp; $0.00088 $ &amp; $ 0.00007 $ &amp; $ 0.00006 $ &amp; $ 0.00004$ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $5.5-6.5$ &amp; $0.201 $ &amp; $ 0.099 $ &amp; $ 0.027 $ &amp; $ 0.008$ \\ $6.5-8.0$ &amp; $0.083 $ &amp; $ 0.010 $ &amp; $ 0.003 $ &amp; $ 0.003$ \\ $8.0-9.0$ &amp; $0.035 $ &amp; $ 0.005 $ &amp; $ 0.003 $ &amp; $ 0.001$ \\ $9.0-10.0$ &amp; $0.028 $ &amp; $ 0.004 $ &amp; $ 0.004 $ &amp; $ 0.001$ \\ $10.0-12.0$ &amp; $0.0152 $ &amp; $ 0.0018 $ &amp; $ 0.0015 $ &amp; $ 0.0006$ \\ $12.0-15.0$ &amp; $0.0065 $ &amp; $ 0.0008 $ &amp; $ 0.0009 $ &amp; $ 0.0003$ \\ $15.0-30.0$ &amp; $0.00136 $ &amp; $ 0.00013 $ &amp; $ 0.00011 $ &amp; $ 0.00005$ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.4 $} \\ \hline $5.5-6.5$ &amp; $0.12 $ &amp; $ 0.04 $ &amp; $ 0.05 $ &amp; $ -0.00$ \\ $6.5-8.0$ &amp; $0.044 $ &amp; $ 0.007 $ &amp; $ 0.008 $ &amp; $ 0.002$ \\ $8.0-9.0$ &amp; $0.033 $ &amp; $ 0.005 $ &amp; $ 0.005 $ &amp; $ 0.001$ \\ $9.0-10.0$ &amp; $0.021 $ &amp; $ 0.004 $ &amp; $ 0.004 $ &amp; $ 0.001$ \\ $10.0-12.0$ &amp; $0.0129 $ &amp; $ 0.0017 $ &amp; $ 0.0019 $ &amp; $ 0.0005$ \\ $12.0-15.0$ &amp; $0.0053 $ &amp; $ 0.0006 $ &amp; $ 0.0005 $ &amp; $ 0.0002$ \\ $15.0-30.0$ &amp; $0.00075 $ &amp; $ 0.00010 $ &amp; $ 0.00007 $ &amp; $ 0.00003$ \\ \hline \end{tabular} \end{table}

"Visible" J/psi cross section (NOT divided by unpolarized acceptance)

Prompt
 \begin{table}[htdp] \begin{tabular}{lcccc} \hline $p_T$ (GeV/c)   &amp;   $\langle A_{\mu\mu} \rangle \cdot \frac{d^2\sigma}{dp_\mathrm{T}dy} \cdot  \mbox{BR} \cdot (1-f_b)$   &amp;   $\pm \sigma_{\mathrm{stat}} $   &amp;   $\pm \sigma_{\mathrm{syst}} $ &amp; $\pm \sigma_{\mathrm{lumi}}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 0.9 $} \\ \hline $8.0-9.0$ &amp; $0.236 $ &amp; $ 0.006 $ &amp; $ 0.006 $ &amp; $ 0.009$ \\ $9.0-10.0$ &amp; $0.291 $ &amp; $ 0.006 $ &amp; $ 0.017 $ &amp; $ 0.012$ \\ $10.0-11.0$ &amp; $0.254 $ &amp; $ 0.005 $ &amp; $ 0.012 $ &amp; $ 0.010$ \\ $11.0-12.0$ &amp; $0.200 $ &amp; $ 0.004 $ &amp; $ 0.008 $ &amp; $ 0.008$ \\ $12.0-13.5$ &amp; $0.138 $ &amp; $ 0.002 $ &amp; $ 0.005 $ &amp; $ 0.006$ \\ $13.5-15.0$ &amp; $0.0856 $ &amp; $ 0.0018 $ &amp; $ 0.0025 $ &amp; $ 0.0034$ \\ $15.0-18.0$ &amp; $0.0454 $ &amp; $ 0.0008 $ &amp; $ 0.0013 $ &amp; $ 0.0018$ \\ $18.0-30.0$ &amp; $0.0093 $ &amp; $ 0.0002 $ &amp; $ 0.0003 $ &amp; $ 0.0004$ \\ $30.0-45.0$ &amp; $0.00078 $ &amp; $ 0.00003 $ &amp; $ 0.00003 $ &amp; $ 0.00003$ \\ $45.0-70.0$ &amp; $0.000070 $ &amp; $ 0.000007 $ &amp; $ 0.000017 $ &amp; $ 0.000003$ \\ \hline \multicolumn{5}{c}{$0.9 < |y| < 1.2 $} \\ \hline $8.0-9.0$ &amp; $0.396 $ &amp; $ 0.012 $ &amp; $ 0.023 $ &amp; $ 0.016$ \\ $9.0-10.0$ &amp; $0.369 $ &amp; $ 0.011 $ &amp; $ 0.029 $ &amp; $ 0.015$ \\ $10.0-12.0$ &amp; $0.254 $ &amp; $ 0.006 $ &amp; $ 0.013 $ &amp; $ 0.010$ \\ $12.0-15.0$ &amp; $0.117 $ &amp; $ 0.003 $ &amp; $ 0.006 $ &amp; $ 0.005$ \\ $15.0-30.0$ &amp; $0.0168 $ &amp; $ 0.0004 $ &amp; $ 0.0004 $ &amp; $ 0.0007$ \\ $30.0-45.0$ &amp; $0.00067 $ &amp; $ 0.00006 $ &amp; $ 0.00005 $ &amp; $ 0.00003$ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $6.5-7.0$ &amp; $0.268 $ &amp; $ 0.017 $ &amp; $ 0.011 $ &amp; $ 0.011$ \\ $7.0-7.5$ &amp; $0.377 $ &amp; $ 0.017 $ &amp; $ 0.008 $ &amp; $ 0.015$ \\ $7.5-8.0$ &amp; $0.546 $ &amp; $ 0.021 $ &amp; $ 0.016 $ &amp; $ 0.022$ \\ $8.0-8.5$ &amp; $0.539 $ &amp; $ 0.019 $ &amp; $ 0.019 $ &amp; $ 0.022$ \\ $8.5-9.0$ &amp; $0.51 $ &amp; $ 0.02 $ &amp; $ 0.03 $ &amp; $ 0.02$ \\ $9.0-10.0$ &amp; $0.429 $ &amp; $ 0.011 $ &amp; $ 0.017 $ &amp; $ 0.017$ \\ $10.0-11.0$ &amp; $0.308 $ &amp; $ 0.008 $ &amp; $ 0.012 $ &amp; $ 0.012$ \\ $11.0-12.0$ &amp; $0.221 $ &amp; $ 0.006 $ &amp; $ 0.008 $ &amp; $ 0.009$ \\ $12.0-15.0$ &amp; $0.116 $ &amp; $ 0.002 $ &amp; $ 0.004 $ &amp; $ 0.005$ \\ $15.0-30.0$ &amp; $0.0155 $ &amp; $ 0.0003 $ &amp; $ 0.0005 $ &amp; $ 0.0006$ \\ $30.0-45.0$ &amp; $0.00080 $ &amp; $ 0.00008 $ &amp; $ 0.00006 $ &amp; $ 0.00003$ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.1 $} \\ \hline $6.5-7.0$ &amp; $0.464 $ &amp; $ 0.025 $ &amp; $ 0.026 $ &amp; $ 0.019$ \\ $7.0-7.25$ &amp; $0.58 $ &amp; $ 0.04 $ &amp; $ 0.03 $ &amp; $ 0.02$ \\ $7.25-7.5$ &amp; $0.62 $ &amp; $ 0.04 $ &amp; $ 0.03 $ &amp; $ 0.02$ \\ $7.5-8.0$ &amp; $0.63 $ &amp; $ 0.03 $ &amp; $ 0.04 $ &amp; $ 0.03$ \\ $8.0-8.5$ &amp; $0.61 $ &amp; $ 0.02 $ &amp; $ 0.03 $ &amp; $ 0.02$ \\ $8.5-9.0$ &amp; $0.576 $ &amp; $ 0.023 $ &amp; $ 0.023 $ &amp; $ 0.023$ \\ $9.0-10.0$ &amp; $0.466 $ &amp; $ 0.014 $ &amp; $ 0.020 $ &amp; $ 0.019$ \\ $10.0-11.0$ &amp; $0.314 $ &amp; $ 0.010 $ &amp; $ 0.014 $ &amp; $ 0.013$ \\ $11.0-12.0$ &amp; $0.222 $ &amp; $ 0.008 $ &amp; $ 0.010 $ &amp; $ 0.009$ \\ $12.0-15.0$ &amp; $0.118 $ &amp; $ 0.003 $ &amp; $ 0.005 $ &amp; $ 0.005$ \\ $15.0-30.0$ &amp; $0.0148 $ &amp; $ 0.0004 $ &amp; $ 0.0006 $ &amp; $ 0.0006$ \\ \hline \multicolumn{5}{c}{$2.1 < |y| < 2.4 $} \\ \hline $5.5-8.0$ &amp; $0.121 $ &amp; $ 0.007 $ &amp; $ 0.006 $ &amp; $ 0.005$ \\ $8.0-9.0$ &amp; $0.194 $ &amp; $ 0.015 $ &amp; $ 0.012 $ &amp; $ 0.008$ \\ $9.0-10.0$ &amp; $0.160 $ &amp; $ 0.012 $ &amp; $ 0.013 $ &amp; $ 0.006$ \\ $10.0-12.0$ &amp; $0.114 $ &amp; $ 0.007 $ &amp; $ 0.012 $ &amp; $ 0.005$ \\ $12.0-15.0$ &amp; $0.055 $ &amp; $ 0.003 $ &amp; $ 0.004 $ &amp; $ 0.002$ \\ $15.0-30.0$ &amp; $0.0077 $ &amp; $ 0.0005 $ &amp; $ 0.0006 $ &amp; $ 0.0003$ \\ \hline \end{tabular} \end{table}

Non Prompt
 \begin{table}[htdp] \begin{tabular}{lcccc} \hline $p_T$ (GeV/c)   &amp;   $\langle A_{\mu\mu} \rangle \cdot \frac{d^2\sigma}{dp_\mathrm{T}dy} \cdot  \mbox{BR} \cdot f_b$   &amp;   $\pm \sigma_{\mathrm{stat}} $   &amp;   $\pm \sigma_{\mathrm{syst}} $ &amp; $\pm \sigma_{\mathrm{lumi}}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 0.9 $} \\ \hline $8.0-9.0$ &amp; $0.0877 $ &amp; $ 0.0023 $ &amp; $ 0.0023 $ &amp; $ 0.0035$ \\ $9.0-10.0$ &amp; $0.116 $ &amp; $ 0.002 $ &amp; $ 0.007 $ &amp; $ 0.005$ \\ $10.0-11.0$ &amp; $0.119 $ &amp; $ 0.002 $ &amp; $ 0.006 $ &amp; $ 0.005$ \\ $11.0-12.0$ &amp; $0.105 $ &amp; $ 0.002 $ &amp; $ 0.005 $ &amp; $ 0.004$ \\ $12.0-13.5$ &amp; $0.082 $ &amp; $ 0.001 $ &amp; $ 0.003 $ &amp; $ 0.003$ \\ $13.5-15.0$ &amp; $0.0612 $ &amp; $ 0.0013 $ &amp; $ 0.0018 $ &amp; $ 0.0024$ \\ $15.0-18.0$ &amp; $0.0378 $ &amp; $ 0.0007 $ &amp; $ 0.0011 $ &amp; $ 0.0015$ \\ $18.0-30.0$ &amp; $0.0107 $ &amp; $ 0.0002 $ &amp; $ 0.0004 $ &amp; $ 0.0004$ \\ $30.0-45.0$ &amp; $0.00134 $ &amp; $ 0.00006 $ &amp; $ 0.00005 $ &amp; $ 0.00005$ \\ $45.0-70.0$ &amp; $0.00013 $ &amp; $ 0.00001 $ &amp; $ 0.00003 $ &amp; $ 0.00001$ \\ \hline \multicolumn{5}{c}{$0.9 < |y| < 1.2 $} \\ \hline $8.0-9.0$ &amp; $0.142 $ &amp; $ 0.004 $ &amp; $ 0.009 $ &amp; $ 0.006$ \\ $9.0-10.0$ &amp; $0.144 $ &amp; $ 0.004 $ &amp; $ 0.012 $ &amp; $ 0.006$ \\ $10.0-12.0$ &amp; $0.122 $ &amp; $ 0.003 $ &amp; $ 0.007 $ &amp; $ 0.005$ \\ $12.0-15.0$ &amp; $0.071 $ &amp; $ 0.002 $ &amp; $ 0.004 $ &amp; $ 0.003$ \\ $15.0-30.0$ &amp; $0.0155 $ &amp; $ 0.0004 $ &amp; $ 0.0004 $ &amp; $ 0.0006$ \\ $30.0-45.0$ &amp; $0.00107 $ &amp; $ 0.00009 $ &amp; $ 0.00006 $ &amp; $ 0.00004$ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $6.5-7.0$ &amp; $0.070 $ &amp; $ 0.004 $ &amp; $ 0.004 $ &amp; $ 0.003$ \\ $7.0-7.5$ &amp; $0.107 $ &amp; $ 0.005 $ &amp; $ 0.004 $ &amp; $ 0.004$ \\ $7.5-8.0$ &amp; $0.153 $ &amp; $ 0.006 $ &amp; $ 0.009 $ &amp; $ 0.006$ \\ $8.0-8.5$ &amp; $0.169 $ &amp; $ 0.006 $ &amp; $ 0.009 $ &amp; $ 0.007$ \\ $8.5-9.0$ &amp; $0.172 $ &amp; $ 0.006 $ &amp; $ 0.012 $ &amp; $ 0.007$ \\ $9.0-10.0$ &amp; $0.162 $ &amp; $ 0.004 $ &amp; $ 0.008 $ &amp; $ 0.006$ \\ $10.0-11.0$ &amp; $0.132 $ &amp; $ 0.004 $ &amp; $ 0.006 $ &amp; $ 0.005$ \\ $11.0-12.0$ &amp; $0.112 $ &amp; $ 0.003 $ &amp; $ 0.005 $ &amp; $ 0.004$ \\ $12.0-15.0$ &amp; $0.0697 $ &amp; $ 0.0014 $ &amp; $ 0.0028 $ &amp; $ 0.0028$ \\ $15.0-30.0$ &amp; $0.0135 $ &amp; $ 0.0003 $ &amp; $ 0.0005 $ &amp; $ 0.0005$ \\ $30.0-45.0$ &amp; $0.00113 $ &amp; $ 0.00011 $ &amp; $ 0.00006 $ &amp; $ 0.00005$ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.1 $} \\ \hline $6.5-7.0$ &amp; $0.115 $ &amp; $ 0.006 $ &amp; $ 0.010 $ &amp; $ 0.005$ \\ $7.0-7.25$ &amp; $0.170 $ &amp; $ 0.010 $ &amp; $ 0.011 $ &amp; $ 0.007$ \\ $7.25-7.5$ &amp; $0.196 $ &amp; $ 0.011 $ &amp; $ 0.013 $ &amp; $ 0.008$ \\ $7.5-8.0$ &amp; $0.193 $ &amp; $ 0.008 $ &amp; $ 0.015 $ &amp; $ 0.008$ \\ $8.0-8.5$ &amp; $0.191 $ &amp; $ 0.008 $ &amp; $ 0.015 $ &amp; $ 0.008$ \\ $8.5-9.0$ &amp; $0.192 $ &amp; $ 0.008 $ &amp; $ 0.013 $ &amp; $ 0.008$ \\ $9.0-10.0$ &amp; $0.162 $ &amp; $ 0.005 $ &amp; $ 0.011 $ &amp; $ 0.006$ \\ $10.0-11.0$ &amp; $0.134 $ &amp; $ 0.004 $ &amp; $ 0.007 $ &amp; $ 0.005$ \\ $11.0-12.0$ &amp; $0.105 $ &amp; $ 0.004 $ &amp; $ 0.007 $ &amp; $ 0.004$ \\ $12.0-15.0$ &amp; $0.065 $ &amp; $ 0.002 $ &amp; $ 0.004 $ &amp; $ 0.003$ \\ $15.0-30.0$ &amp; $0.0125 $ &amp; $ 0.0003 $ &amp; $ 0.0006 $ &amp; $ 0.0005$ \\ \hline \multicolumn{5}{c}{$2.1 < |y| < 2.4 $} \\ \hline $5.5-8.0$ &amp; $0.0330 $ &amp; $ 0.0019 $ &amp; $ 0.0026 $ &amp; $ 0.0013$ \\ $8.0-9.0$ &amp; $0.057 $ &amp; $ 0.004 $ &amp; $ 0.006 $ &amp; $ 0.002$ \\ $9.0-10.0$ &amp; $0.061 $ &amp; $ 0.005 $ &amp; $ 0.006 $ &amp; $ 0.002$ \\ $10.0-12.0$ &amp; $0.047 $ &amp; $ 0.003 $ &amp; $ 0.005 $ &amp; $ 0.002$ \\ $12.0-15.0$ &amp; $0.0320 $ &amp; $ 0.0017 $ &amp; $ 0.0026 $ &amp; $ 0.0013$ \\ $15.0-30.0$ &amp; $0.0058 $ &amp; $ 0.0003 $ &amp; $ 0.0005 $ &amp; $ 0.0002$ \\ \hline \end{tabular} \end{table}

For the non-prompt J/psi, in order to ease comparison with NLO MC generators we also provide the total cross section in the visible region of the phase space R:

 \begin{eqnarray} \nonumber {\cal B}(J/\psi \rightarrow \mu^+ \mu^-) \cdot \sigma(pp \rightarrow b {\bar b} \rightarrow J/\psi X)_R = 4.67 \pm 0.08 \mathrm{(stat)} \pm 0.17 \mathrm{(syst)} \pm 0.19 \mathrm{(lumi)~nb} \end{eqnarray}

where R is defined by the single muon criteria:

 \begin{eqnarray} \nonumber |\eta^\mu|<1.2    &amp;\rightarrow \quad  p_{T}^{\mu}>4.0~\mathrm{GeV}/c \quad, \\ \nonumber 1.2 < |\eta^\mu|<2.4    &amp;\rightarrow \quad  p_{T}^{\mu}>3.3~\mathrm{GeV}/c \quad. \end{eqnarray}

and the J/psi criteria:

 \begin{eqnarray} \nonumber |y^{J/\psi}|<1.2    &amp;\rightarrow \quad  p_{T}^{J/\psi}>8.0~\mathrm{GeV}/c \quad, \\ \nonumber 1.2 < |y^{J/\psi}|<2.1    &amp;\rightarrow \quad  p_{T}^{J/\psi}>6.5~\mathrm{GeV}/c \quad, \\ \nonumber 2.1 < |y^{J/\psi}|<2.4    &amp;\rightarrow \quad  p_{T}^{J/\psi}>5.5~\mathrm{GeV}/c \quad.  \end{eqnarray}

"Visible" psi(2S) cross section (NOT divided by unpolarized acceptance)

Prompt
 \begin{table}[htdp] \begin{tabular}{lcccc} \hline $p_T$ (GeV/c)   &amp;   $\langle A_{\mu\mu} \rangle \cdot \frac{d^2\sigma}{dp_\mathrm{T}dy} \cdot  \mbox{BR} \cdot (1-f_b)$   &amp;   $\pm \sigma_{\mathrm{stat}} $   &amp;   $\pm \sigma_{\mathrm{syst}} $ &amp; $\pm \sigma_{\mathrm{lumi}}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 1.2 $} \\ \hline $6.5-8.0$ &amp; $0.0039 $ &amp; $ 0.0008 $ &amp; $ 0.0005 $ &amp; $ 0.0002$ \\ $8.0-9.0$ &amp; $0.0098 $ &amp; $ 0.0010 $ &amp; $ 0.0007 $ &amp; $ 0.0004$ \\ $9.0-10.0$ &amp; $0.0127 $ &amp; $ 0.0011 $ &amp; $ 0.0008 $ &amp; $ 0.0005$ \\ $10.0-11.0$ &amp; $0.0104 $ &amp; $ 0.0009 $ &amp; $ 0.0007 $ &amp; $ 0.0004$ \\ $11.0-12.0$ &amp; $0.0075 $ &amp; $ 0.0007 $ &amp; $ 0.0008 $ &amp; $ 0.0003$ \\ $12.0-13.5$ &amp; $0.0059 $ &amp; $ 0.0004 $ &amp; $ 0.0004 $ &amp; $ 0.0002$ \\ $13.5-15.0$ &amp; $0.0036 $ &amp; $ 0.0003 $ &amp; $ 0.0003 $ &amp; $ 0.0001$ \\ $15.0-18.0$ &amp; $0.00202 $ &amp; $ 0.00016 $ &amp; $ 0.00009 $ &amp; $ 0.00008$ \\ $18.0-30.0$ &amp; $0.00043 $ &amp; $ 0.00003 $ &amp; $ 0.00003 $ &amp; $ 0.00002$ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $5.5-6.5$ &amp; $0.0109 $ &amp; $ 0.0054 $ &amp; $ 0.0008 $ &amp; $ 0.0004$ \\ $6.5-8.0$ &amp; $0.0154 $ &amp; $ 0.0019 $ &amp; $ 0.0004 $ &amp; $ 0.0006$ \\ $8.0-9.0$ &amp; $0.0163 $ &amp; $ 0.0023 $ &amp; $ 0.0010 $ &amp; $ 0.0007$ \\ $9.0-10.0$ &amp; $0.0167 $ &amp; $ 0.0025 $ &amp; $ 0.0016 $ &amp; $ 0.0007$ \\ $10.0-12.0$ &amp; $0.0103 $ &amp; $ 0.0012 $ &amp; $ 0.0008 $ &amp; $ 0.0004$ \\ $12.0-15.0$ &amp; $0.0055 $ &amp; $ 0.0006 $ &amp; $ 0.0007 $ &amp; $ 0.0002$ \\ $15.0-30.0$ &amp; $0.00088 $ &amp; $ 0.00009 $ &amp; $ 0.00008 $ &amp; $ 0.00004$ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.4 $} \\ \hline $5.5-6.5$ &amp; $0.0068 $ &amp; $ 0.0024 $ &amp; $ 0.0020 $ &amp; $ 0.0003$ \\ $6.5-8.0$ &amp; $0.0157 $ &amp; $ 0.0026 $ &amp; $ 0.0011 $ &amp; $ 0.0006$ \\ $8.0-9.0$ &amp; $0.0134 $ &amp; $ 0.0019 $ &amp; $ 0.0013 $ &amp; $ 0.0005$ \\ $9.0-10.0$ &amp; $0.0115 $ &amp; $ 0.0020 $ &amp; $ 0.0017 $ &amp; $ 0.0005$ \\ $10.0-12.0$ &amp; $0.0073 $ &amp; $ 0.0009 $ &amp; $ 0.0009 $ &amp; $ 0.0003$ \\ $12.0-15.0$ &amp; $0.0039 $ &amp; $ 0.0005 $ &amp; $ 0.0003 $ &amp; $ 0.0002$ \\ $15.0-30.0$ &amp; $0.00055 $ &amp; $ 0.00007 $ &amp; $ 0.00005 $ &amp; $ 0.00002$ \\ \hline \end{tabular} \end{table}

Non Prompt
 \begin{table}[htdp] \begin{tabular}{lcccc} \hline $p_T$ (GeV/c)   &amp;   $\langle A_{\mu\mu} \rangle \cdot \frac{d^2\sigma}{dp_\mathrm{T}dy} \cdot  \mbox{BR} \cdot f_b$   &amp;   $\pm \sigma_{\mathrm{stat}} $   &amp;   $\pm \sigma_{\mathrm{syst}} $ &amp; $\pm \sigma_{\mathrm{lumi}}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 1.2 $} \\ \hline $6.5-8.0$ &amp; $0.00188 $ &amp; $ 0.00036 $ &amp; $ 0.00026 $ &amp; $ 0.00008$ \\ $8.0-9.0$ &amp; $0.0053 $ &amp; $ 0.0005 $ &amp; $ 0.0004 $ &amp; $ 0.0002$ \\ $9.0-10.0$ &amp; $0.0064 $ &amp; $ 0.0005 $ &amp; $ 0.0005 $ &amp; $ 0.0003$ \\ $10.0-11.0$ &amp; $0.0063 $ &amp; $ 0.0005 $ &amp; $ 0.0005 $ &amp; $ 0.0003$ \\ $11.0-12.0$ &amp; $0.0049 $ &amp; $ 0.0004 $ &amp; $ 0.0006 $ &amp; $ 0.0002$ \\ $12.0-13.5$ &amp; $0.0044 $ &amp; $ 0.0003 $ &amp; $ 0.0003 $ &amp; $ 0.0002$ \\ $13.5-15.0$ &amp; $0.00304 $ &amp; $ 0.00027 $ &amp; $ 0.00027 $ &amp; $ 0.00012$ \\ $15.0-18.0$ &amp; $0.00192 $ &amp; $ 0.00015 $ &amp; $ 0.00009 $ &amp; $ 0.00008$ \\ $18.0-30.0$ &amp; $0.00058 $ &amp; $ 0.00004 $ &amp; $ 0.00003 $ &amp; $ 0.00002$ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $5.5-6.5$ &amp; $0.0036 $ &amp; $ 0.0018 $ &amp; $ 0.0005 $ &amp; $ 0.0001$ \\ $6.5-8.0$ &amp; $0.00687 $ &amp; $ 0.00085 $ &amp; $ 0.00028 $ &amp; $ 0.00027$ \\ $8.0-9.0$ &amp; $0.0073 $ &amp; $ 0.0010 $ &amp; $ 0.0007 $ &amp; $ 0.0003$ \\ $9.0-10.0$ &amp; $0.0080 $ &amp; $ 0.0012 $ &amp; $ 0.0011 $ &amp; $ 0.0003$ \\ $10.0-12.0$ &amp; $0.0060 $ &amp; $ 0.0007 $ &amp; $ 0.0006 $ &amp; $ 0.0002$ \\ $12.0-15.0$ &amp; $0.0033 $ &amp; $ 0.0004 $ &amp; $ 0.0005 $ &amp; $ 0.0001$ \\ $15.0-30.0$ &amp; $0.00092 $ &amp; $ 0.00009 $ &amp; $ 0.00008 $ &amp; $ 0.00004$ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.4 $} \\ \hline $5.5-6.5$ &amp; $0.0018 $ &amp; $ 0.0007 $ &amp; $ 0.0008 $ &amp; $ 0.0001$ \\ $6.5-8.0$ &amp; $0.0038 $ &amp; $ 0.0006 $ &amp; $ 0.0006 $ &amp; $ 0.0002$ \\ $8.0-9.0$ &amp; $0.0057 $ &amp; $ 0.0008 $ &amp; $ 0.0008 $ &amp; $ 0.0002$ \\ $9.0-10.0$ &amp; $0.0049 $ &amp; $ 0.0008 $ &amp; $ 0.0010 $ &amp; $ 0.0002$ \\ $10.0-12.0$ &amp; $0.0043 $ &amp; $ 0.0006 $ &amp; $ 0.0006 $ &amp; $ 0.0002$ \\ $12.0-15.0$ &amp; $0.00230 $ &amp; $ 0.00027 $ &amp; $ 0.00022 $ &amp; $ 0.00009$ \\ $15.0-30.0$ &amp; $0.00044 $ &amp; $ 0.00006 $ &amp; $ 0.00004 $ &amp; $ 0.00002$ \\ \hline \end{tabular} \end{table}

Cross section ratios

Prompt

 \begin{table}[htdp] \begin{tabular}{lcccc} \hline $p_T~({\rm GeV}/c)$  &amp; $\frac{\frac{d^2\sigma}{dp_\mathrm{T}dy}(\psi{\rm (2S)}) \cdot  \mbox{BR}(\psi{\rm (2S)}\rightarrow \mu^{+}\mu^{-})}{\frac{d^2\sigma}{dp_\mathrm{T}dy}(J/\psi) \cdot  \mbox{BR}(J/\psi \rightarrow \mu^{+}\mu^{-})}$  &amp; $\pm \sigma_{\rm stat}$  &amp; $\pm \sigma_{\rm syst}$ &amp; $\pm \sigma_{\rm pol}$ \\ \hline \multicolumn{5}{c}{$|y| < 1.2$} \\ \hline $8-9$ &amp; $0.0308 $ &amp; $ 0.0014 $ &amp; $ 0.0018 $   &amp; $^{+0.005}_{-0.006}$\\ $9-10$ &amp; $0.0370 $ &amp; $ 0.0015 $ &amp; $ 0.0019 $  &amp; $^{+0.006}_{-0.006}$\\ $10-11$ &amp; $0.0351 $ &amp; $ 0.0015 $ &amp; $ 0.0015 $ &amp; $^{+0.006}_{-0.006}$\\ $11-12$ &amp; $0.0369 $ &amp; $ 0.0017 $ &amp; $ 0.0015 $ &amp; $^{+0.007}_{-0.007}$\\ $12-13$ &amp; $0.0408 $ &amp; $ 0.0016 $ &amp; $ 0.0018 $ &amp; $^{+0.006}_{-0.007}$\\ $13-15$ &amp; $0.0442 $ &amp; $ 0.0021 $ &amp; $ 0.0018 $ &amp; $^{+0.007}_{-0.008}$\\ $15-18$ &amp; $0.0415 $ &amp; $ 0.0019 $ &amp; $ 0.0017 $ &amp; $^{+0.005}_{-0.007}$\\ $18-30$ &amp; $0.0462 $ &amp; $ 0.0021 $ &amp; $ 0.0026 $ &amp; $^{+0.005}_{-0.007}$\\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6$} \\ \hline $6.5-8$ &amp; $0.040 $ &amp; $ 0.002 $ &amp; $ 0.006 $  &amp; $^{+0.006}_{-0.006}$ \\ $8-9$ &amp; $0.033 $ &amp; $ 0.002 $ &amp; $ 0.005 $  &amp; $^{+0.006}_{-0.005}$\\ $9-10$ &amp; $0.041 $ &amp; $ 0.003 $ &amp; $ 0.006 $ &amp; $^{+0.006}_{-0.007}$\\ $10-12$ &amp; $0.039 $ &amp; $ 0.003 $ &amp; $ 0.006 $&amp; $^{+0.005}_{-0.007}$ \\ $12-15$ &amp; $0.054 $ &amp; $ 0.005 $ &amp; $ 0.010 $&amp; $^{+0.008}_{-0.008}$ \\ $15-30$ &amp; $0.055 $ &amp; $ 0.003 $ &amp; $ 0.008 $&amp; $^{+0.006}_{-0.008}$ \\ \hline					       \multicolumn{5}{c}{$1.6 < |y| < 2.4$} \\ \hline $6.5-8$ &amp; $0.039 $ &amp; $ 0.003 $ &amp; $ 0.003 $     &amp; $^{+0.005}_{-0.007}$\\ $8-9$ &amp; $0.0302 $ &amp; $ 0.0024 $ &amp; $ 0.0018 $  &amp; $^{+0.005}_{-0.006}$\\ $9-10$ &amp; $0.040 $ &amp; $ 0.004 $ &amp; $ 0.004 $    &amp; $^{+0.006}_{-0.007}$\\ $10-12$ &amp; $0.0317 $ &amp; $ 0.0023 $ &amp; $ 0.0019 $&amp; $^{+0.005}_{-0.006}$ \\ $12-15$ &amp; $0.0406 $ &amp; $ 0.0028 $ &amp; $ 0.0023 $&amp; $^{+0.005}_{-0.007}$ \\ $15-30$ &amp; $0.0443 $ &amp; $ 0.0038 $ &amp; $ 0.0020 $&amp; $^{+0.005}_{-0.008}$ \\ \hline		 \multicolumn{5}{c}{Integrated: $|y| < 2.4$} \\ \hline $6.5-8$ &amp; $0.0358 $ &amp; $ 0.0017 $ &amp; $ 0.0039 $ &amp; $^{+0.006}_{-0.007}$\\ $8-9$ &amp; $0.0323 $ &amp; $ 0.0013 $ &amp; $ 0.0024 $   &amp; $^{+0.005}_{-0.006}$\\ $9-10$ &amp; $0.0367 $ &amp; $ 0.0016 $ &amp; $ 0.0027 $  &amp; $^{+0.006}_{-0.006}$\\ $10-12$ &amp; $0.0355 $ &amp; $ 0.0010 $ &amp; $ 0.0026 $  &amp; $^{+0.006}_{-0.006}$\\ $12-15$ &amp; $0.0422 $ &amp; $ 0.0013 $ &amp; $ 0.0032 $ &amp; $^{+0.006}_{-0.008}$\\ $15-30$ &amp; $0.0441 $ &amp; $ 0.0013 $ &amp; $ 0.0035 $ &amp; $^{+0.005}_{-0.007}$\\  \hline \end{tabular} \end{table}

Non prompt

 \begin{table}[htdp] \begin{tabular}{lccc} \hline $p_T~({\rm GeV}/c)$ &amp; $\frac{\frac{d^2\sigma}{dp_\mathrm{T}dy}(\psi{\rm (2S)}) \cdot  \mbox{BR}(\psi{\rm (2S)} \rightarrow \mu^{+}\mu^{-})}{\frac{d^2\sigma}{dp_\mathrm{T}dy}(J/\psi) \cdot  \mbox{BR}(J/\psi \rightarrow \mu^{+}\mu^{-})}$  &amp; $\pm \sigma_{\rm stat}$  &amp; $\pm \sigma_{\rm syst}$ \\ \hline \multicolumn{4}{c}{$|y| < 1.2$} \\ \hline $8-9$ &amp; $0.0480 $ &amp; $ 0.0022 $ &amp; $ 0.0028 $  \\ $9-10$ &amp; $0.0483 $ &amp; $ 0.0019 $ &amp; $ 0.0024 $  \\ $10-11$ &amp; $0.0452 $ &amp; $ 0.0019 $ &amp; $ 0.0020 $  \\ $11-12$ &amp; $0.0466 $ &amp; $ 0.0021 $ &amp; $ 0.0019 $  \\ $12-13$ &amp; $0.0519 $ &amp; $ 0.0021 $ &amp; $ 0.0023 $  \\ $13-15$ &amp; $0.0527 $ &amp; $ 0.0025 $ &amp; $ 0.0021 $  \\ $15-18$ &amp; $0.0475 $ &amp; $ 0.0022 $ &amp; $ 0.0019 $  \\ $18-30$ &amp; $0.054 $ &amp; $ 0.002 $ &amp; $ 0.003 $  \\ \hline \multicolumn{4}{c}{$1.2 < |y| < 1.6$} \\ \hline $6.5-8$ &amp; $0.054 $ &amp; $ 0.003 $ &amp; $ 0.008 $  \\ $8-9$ &amp; $0.042 $ &amp; $ 0.003 $ &amp; $ 0.006 $  \\ $9-10$ &amp; $0.047 $ &amp; $ 0.004 $ &amp; $ 0.007 $  \\ $10-12$ &amp; $0.047 $ &amp; $ 0.003 $ &amp; $ 0.007 $  \\ $12-15$ &amp; $0.049 $ &amp; $ 0.005 $ &amp; $ 0.009 $  \\ $15-30$ &amp; $0.063 $ &amp; $ 0.003 $ &amp; $ 0.009 $  \\ \hline \multicolumn{4}{c}{$1.6 < |y| < 2.4$} \\ \hline $6.5-8$ &amp; $0.0318 $ &amp; $ 0.0023 $ &amp; $ 0.0029 $  \\ $8-9$ &amp; $0.0435 $ &amp; $ 0.0034 $ &amp; $ 0.0027 $  \\ $9-10$ &amp; $0.042 $ &amp; $ 0.004 $ &amp; $ 0.004 $  \\ $10-12$ &amp; $0.0468 $ &amp; $ 0.0034 $ &amp; $ 0.0029 $  \\ $12-15$ &amp; $0.0446 $ &amp; $ 0.0031 $ &amp; $ 0.0025 $  \\ $15-30$ &amp; $0.0451 $ &amp; $ 0.0039 $ &amp; $ 0.0021 $  \\  \hline \multicolumn{4}{c}{Integrated: $|y| < 2.4$} \\ \hline $6.5-8$ &amp; $0.0390 $ &amp; $ 0.0031 $ &amp; $ 0.0052 $ \\ $8-9$ &amp; $0.0455 $ &amp; $ 0.0026 $ &amp; $ 0.0033 $ \\ $9-10$ &amp; $0.0470 $ &amp; $ 0.0032 $ &amp; $ 0.0034 $ \\ $10-12$ &amp; $0.0460 $ &amp; $ 0.0022 $ &amp; $ 0.0033 $ \\ $12-15$ &amp; $0.0504 $ &amp; $ 0.0022 $ &amp; $ 0.0033 $ \\ $15-30$ &amp; $0.0499 $ &amp; $ 0.0020 $ &amp; $ 0.0040 $ \\  \hline \end{tabular} \end{table}

Non-prompt fractions

Fraction of J/psi from b-hadrons in pT and |y| bins. The b-fraction column shows the statistical and systematic errors.

 \begin{table}[h!] \begin{tabular}{llc} \hline $|y|$ &amp; $p_T~({\rm GeV}/c)$  &amp; $f_B(J/\psi)$ \\ \hline $0.0-0.9$ &amp; $8.0-9.0$ &amp; $0.271 \pm 0.006 \pm 0.003$ \\ &amp; $9.0-10.0$ &amp; $0.285 \pm 0.005 \pm 0.004$ \\ &amp; $10.0-11.0$ &amp; $0.320 \pm 0.005 \pm 0.004$ \\ &amp; $11.0-12.0$ &amp; $0.345 \pm 0.005 \pm 0.007$ \\ &amp; $12.0-13.5$ &amp; $0.373 \pm 0.005 \pm 0.003$ \\ &amp; $13.5-15.0$ &amp; $0.417 \pm 0.006 \pm 0.005$ \\ &amp; $15.0-18.0$ &amp; $0.454 \pm 0.006 \pm 0.004$ \\ &amp; $18.0-30.0$ &amp; $0.535 \pm 0.006 \pm 0.004$ \\ &amp; $30.0-45.0$ &amp; $0.633 \pm 0.015 \pm 0.010$ \\ &amp; $45.0-70.0$ &amp; $0.646 \pm 0.038 \pm 0.024$ \\ \hline $0.9-1.2$ &amp; $8.0-9.0$ &amp; $0.265 \pm 0.007 \pm 0.007$ \\ &amp; $9.0-10.0$ &amp; $0.281 \pm 0.007 \pm 0.007$ \\ &amp; $10.0-12.0$ &amp; $0.324 \pm 0.006 \pm 0.007$ \\ &amp; $12.0-15.0$ &amp; $0.380 \pm 0.006 \pm 0.008$ \\ &amp; $15.0-30.0$ &amp; $0.481 \pm 0.007 \pm 0.007$ \\ &amp; $30.0-45.0$ &amp; $0.616 \pm 0.029 \pm 0.028$ \\ \hline $1.2-1.6$ &amp; $6.5-7.0$ &amp; $0.207 \pm 0.010 \pm 0.006$ \\ &amp; $7.0-7.5$ &amp; $0.221 \pm 0.009 \pm 0.006$ \\ &amp; $7.5-8.0$ &amp; $0.219 \pm 0.007 \pm 0.012$ \\ &amp; $8.0-8.5$ &amp; $0.238 \pm 0.007 \pm 0.011$ \\ &amp; $8.5-9.0$ &amp; $0.253 \pm 0.007 \pm 0.009$ \\ &amp; $9.0-10.0$ &amp; $0.275 \pm 0.006 \pm 0.008$ \\ &amp; $10.0-11.0$ &amp; $0.299 \pm 0.006 \pm 0.009$ \\ &amp; $11.0-12.0$ &amp; $0.335 \pm 0.007 \pm 0.009$ \\ &amp; $12.0-15.0$ &amp; $0.376 \pm 0.006 \pm 0.011$ \\ &amp; $15.0-30.0$ &amp; $0.466 \pm 0.007 \pm 0.013$ \\ &amp; $30.0-45.0$ &amp; $0.583 \pm 0.026 \pm 0.024$ \\ \hline $1.6-2.1$ &amp; $6.50-7.00$ &amp; $0.199 \pm 0.010 \pm 0.012$ \\ &amp; $7.00-7.25$ &amp; $0.225 \pm 0.013 \pm 0.010$ \\ &amp; $7.25-7.50$ &amp; $0.239 \pm 0.013 \pm 0.010$ \\ &amp; $7.50-8.00$ &amp; $0.233 \pm 0.009 \pm 0.013$ \\ &amp; $8.00-8.50$ &amp; $0.237 \pm 0.009 \pm 0.015$ \\ &amp; $8.50-9.00$ &amp; $0.250 \pm 0.009 \pm 0.014$ \\ &amp; $9.00-10.00$ &amp; $0.258 \pm 0.007 \pm 0.014$ \\ &amp; $10.00-11.00$ &amp; $0.299 \pm 0.008 \pm 0.010$ \\ &amp; $11.00-12.00$ &amp; $0.321 \pm 0.010 \pm 0.015$ \\ &amp; $12.00-15.00$ &amp; $0.356 \pm 0.008 \pm 0.017$ \\ &amp; $15.00-30.00$ &amp; $0.458 \pm 0.009 \pm 0.019$ \\ \hline $2.1-2.4$ &amp; $5.5-8.0$ &amp; $0.214 \pm 0.012 \pm 0.013$ \\ &amp; $8.0-9.0$ &amp; $0.226 \pm 0.016 \pm 0.020$ \\ &amp; $9.0-10.0$ &amp; $0.275 \pm 0.018 \pm 0.020$ \\ &amp; $10.0-12.0$ &amp; $0.294 \pm 0.014 \pm 0.018$ \\ &amp; $12.0-15.0$ &amp; $0.368 \pm 0.016 \pm 0.017$ \\ &amp; $15.0-30.0$ &amp; $0.432 \pm 0.020 \pm 0.023$ \\ \hline \end{tabular} \end{table}

Fraction of psi(2S) from b-hadrons in pT and |y| bins. The b-fraction column shows the statistical and systematic errors and the b-fraction ratio over the J/psi is also shown.

 \begin{table}[htdp] \begin{tabular}{llcc} \hline $|y|$ &amp; $p_T$ (GeV/$c$) &amp;  $f_B(\psi{\rm (2S)})$ &amp; $f_B(\psi{\rm (2S)})/f_B(J/\psi)$ \\ \hline $0.0-1.2$ &amp; $6.5-8.0$ &amp; $0.326 \pm 0.041 \pm 0.011$ &amp; $1.46 \pm 0.19 \pm 0.08$ \\ &amp; $8.0-9.0$ &amp; $0.350 \pm 0.025 \pm 0.014$ &amp; $1.30 \pm 0.12 \pm 0.08$ \\ &amp; $9.0-10.0$ &amp; $0.335 \pm 0.021 \pm 0.020$ &amp; $1.20 \pm 0.08 \pm 0.08$ \\ &amp; $10.0-11.0$ &amp; $0.378 \pm 0.023 \pm 0.022$ &amp; $1.19 \pm 0.08 \pm 0.07$ \\ &amp; $11.0-12.0$ &amp; $0.394 \pm 0.024 \pm 0.028$ &amp; $1.16 \pm 0.07 \pm 0.09$ \\ &amp; $12.0-13.5$ &amp; $0.431 \pm 0.022 \pm 0.020$ &amp; $1.16 \pm 0.06 \pm 0.05$ \\ &amp; $13.5-15.0$ &amp; $0.456 \pm 0.025 \pm 0.028$ &amp; $1.10 \pm 0.06 \pm 0.07$ \\ &amp; $15.0-18.0$ &amp; $0.487 \pm 0.024 \pm 0.017$ &amp; $1.08 \pm 0.05 \pm 0.04$ \\ &amp; $18.0-30.0$ &amp; $0.572 \pm 0.025 \pm 0.028$ &amp; $1.08 \pm 0.05 \pm 0.05$ \\ \hline $1.2-1.6$ &amp; $5.5-6.5$ &amp; $0.246 \pm 0.093 \pm 0.029$ &amp; $1.33 \pm 0.51 \pm 0.22$ \\ &amp; $6.5-8.0$ &amp; $0.308 \pm 0.030 \pm 0.010$ &amp; $1.42 \pm 0.14 \pm 0.07$ \\ &amp; $8.0-9.0$ &amp; $0.309 \pm 0.035 \pm 0.022$ &amp; $1.26 \pm 0.14 \pm 0.11$ \\ &amp; $9.0-10.0$ &amp; $0.32 \pm 0.03 \pm 0.04$ &amp; $1.18 \pm 0.12 \pm 0.14$ \\ &amp; $10.0-12.0$ &amp; $0.366 \pm 0.029 \pm 0.028$ &amp; $1.16 \pm 0.09 \pm 0.09$ \\ &amp; $12.0-15.0$ &amp; $0.375 \pm 0.032 \pm 0.028$ &amp; $1.00 \pm 0.09 \pm 0.07$ \\ &amp; $15.0-30.0$ &amp; $0.51 \pm 0.03 \pm 0.04$ &amp; $1.09 \pm 0.07 \pm 0.08$ \\ \hline $1.6-2.4$ &amp; $5.5-6.5$ &amp; $0.21 \pm 0.06 \pm 0.07$ &amp; $1.2 \pm 0.3 \pm 0.3$ \\ &amp; $6.5-8.0$ &amp; $0.19 \pm 0.03 \pm 0.03$ &amp; $0.88 \pm 0.13 \pm 0.13$ \\ &amp; $8.0-9.0$ &amp; $0.30 \pm 0.04 \pm 0.04$ &amp; $1.24 \pm 0.15 \pm 0.18$ \\ &amp; $9.0-10.0$ &amp; $0.30 \pm 0.04 \pm 0.05$ &amp; $1.14 \pm 0.17 \pm 0.19$ \\ &amp; $10.0-12.0$ &amp; $0.37 \pm 0.03 \pm 0.04$ &amp; $1.23 \pm 0.11 \pm 0.14$ \\ &amp; $12.0-15.0$ &amp; $0.372 \pm 0.035 \pm 0.015$ &amp; $1.04 \pm 0.10 \pm 0.07$ \\ &amp; $15.0-30.0$ &amp; $0.45 \pm 0.04 \pm 0.04$ &amp; $0.97 \pm 0.09 \pm 0.07$ \\ \hline \end{tabular} \end{table}

Variations of prompt cross-sections with extreme polarization scenarios

Cross sections as a function of y and pT, assuming four polarization scenarios, namely fully longitudinal in the Collins-Soper frame (CS_L), fully transverse in the Collins-Soper frame (CS_T), fully longitudinal in the helicity frame (HX_L), fully trasverse in the helicity frame (HX_T). The results are expressed as a difference with respect to the values measured assuming null-polarization and listed in tables above, and are expressed in nb / (GeV/c).

Prompt J/psi

 \begin{table}[h!] \begin{tabular}{lcccc} \hline $p_T$ (GeV/$c$) &amp; $\Delta \sigma {\rm (CS_L)}$ &amp; $\Delta \sigma {\rm (CS_T)}$ &amp; $\Delta \sigma {\rm (HX_L)}$ &amp; $\Delta \sigma {\rm (HX_T)}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 0.9 $} \\ \hline $8.0-9.0 $ &amp; $ 0.21 $ &amp; $ -0.06 $ &amp; $ -0.62 $ &amp; $ 0.58 $ \\ $9.0-10.0 $ &amp; $ 0.22 $ &amp; $ -0.06 $ &amp; $ -0.37 $ &amp; $ 0.31 $ \\ $10.0-11.0 $ &amp; $ 0.155 $ &amp; $ -0.049 $ &amp; $ -0.213 $ &amp; $ 0.170 $ \\ $11.0-12.0 $ &amp; $ 0.085 $ &amp; $ -0.031 $ &amp; $ -0.127 $ &amp; $ 0.087 $ \\ $12.0-13.5 $ &amp; $ 0.037 $ &amp; $ -0.013 $ &amp; $ -0.065 $ &amp; $ 0.050 $ \\ $13.5-15.0 $ &amp; $ 0.022 $ &amp; $ -0.008 $ &amp; $ -0.030 $ &amp; $ 0.020 $ \\ $15.0-18.0 $ &amp; $ 0.0066 $ &amp; $ -0.0027 $ &amp; $ -0.0124 $ &amp; $ 0.0080 $ \\ $18.0-30.0 $ &amp; $ 0.0009 $ &amp; $ -0.0003 $ &amp; $ -0.0015 $ &amp; $ 0.0008 $ \\ $30.0-45.0 $ &amp; $ 0 $ &amp; $ 0 $ &amp; $ 0 $ &amp; $ 0 $ \\ $45.0-70.0 $ &amp; $ 0 $ &amp; $ 0 $ &amp; $ 0 $ &amp; $ 0 $ \\ \hline \multicolumn{5}{c}{$0.9 < |y| < 1.2 $} \\ \hline $8.0-9.0 $ &amp; $ 0.64 $ &amp; $ -0.21 $ &amp; $ -0.61 $ &amp; $ 0.62 $ \\ $9.0-10.0 $ &amp; $ 0.26 $ &amp; $ -0.11 $ &amp; $ -0.36 $ &amp; $ 0.28 $ \\ $10.0-12.0 $ &amp; $ 0.109 $ &amp; $ -0.040 $ &amp; $ -0.156 $ &amp; $ 0.134 $ \\ $12.0-15.0 $ &amp; $ 0.033 $ &amp; $ -0.011 $ &amp; $ -0.040 $ &amp; $ 0.028 $ \\ $15.0-30.0 $ &amp; $ 0.0019 $ &amp; $ -0.0008 $ &amp; $ -0.0034 $ &amp; $ 0.0019 $ \\ $30.0-45.0 $ &amp; $ 0 $ &amp; $ 0 $ &amp; $ 0 $ &amp; $ 0 $ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $6.5-7.0 $ &amp; $ -1.46 $ &amp; $ 1.06 $ &amp; $ -1.90 $ &amp; $ 2.13 $ \\ $7.0-7.5 $ &amp; $ -0.56 $ &amp; $ 0.34 $ &amp; $ -1.25 $ &amp; $ 1.19 $ \\ $7.5-8.0 $ &amp; $ -0.04 $ &amp; $ -0.03 $ &amp; $ -1.05 $ &amp; $ 0.71 $ \\ $8.0-8.5 $ &amp; $ 0.19 $ &amp; $ -0.01 $ &amp; $ -0.70 $ &amp; $ 0.52 $ \\ $8.5-9.0 $ &amp; $ 0.24 $ &amp; $ -0.06 $ &amp; $ -0.51 $ &amp; $ 0.38 $ \\ $9.0-10.0 $ &amp; $ 0.18 $ &amp; $ -0.07 $ &amp; $ -0.33 $ &amp; $ 0.27 $ \\ $10.0-11.0 $ &amp; $ 0.095 $ &amp; $ -0.030 $ &amp; $ -0.174 $ &amp; $ 0.138 $ \\ $11.0-12.0 $ &amp; $ 0.048 $ &amp; $ -0.029 $ &amp; $ -0.104 $ &amp; $ 0.075 $ \\ $12.0-15.0 $ &amp; $ 0.023 $ &amp; $ -0.008 $ &amp; $ -0.039 $ &amp; $ 0.025 $ \\ $15.0-30.0 $ &amp; $ 0.0012 $ &amp; $ -0.0007 $ &amp; $ -0.0026 $ &amp; $ 0.0017 $ \\ $30.0-45.0 $ &amp; $ 0 $ &amp; $ 0 $ &amp; $ 0 $ &amp; $ 0 $ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.1 $} \\ \hline $6.5-7.0 $ &amp; $ -0.17 $ &amp; $ 0.18 $ &amp; $ -2.22 $ &amp; $ 2.26 $ \\ $7.0-7.25 $ &amp; $ 0.71 $ &amp; $ 0.09 $ &amp; $ -1.54 $ &amp; $ 1.33 $ \\ $7.25-7.5 $ &amp; $ 0.77 $ &amp; $ -0.23 $ &amp; $ -1.19 $ &amp; $ 1.01 $ \\ $7.5-8.0 $ &amp; $ 0.57 $ &amp; $ -0.13 $ &amp; $ -0.98 $ &amp; $ 0.70 $ \\ $8.0-8.5 $ &amp; $ 0.51 $ &amp; $ -0.14 $ &amp; $ -0.69 $ &amp; $ 0.55 $ \\ $8.5-9.0 $ &amp; $ 0.43 $ &amp; $ -0.12 $ &amp; $ -0.53 $ &amp; $ 0.44 $ \\ $9.0-10.0 $ &amp; $ 0.23 $ &amp; $ -0.08 $ &amp; $ -0.33 $ &amp; $ 0.26 $ \\ $10.0-11.0 $ &amp; $ 0.118 $ &amp; $ -0.056 $ &amp; $ -0.182 $ &amp; $ 0.144 $ \\ $11.0-12.0 $ &amp; $ 0.065 $ &amp; $ -0.023 $ &amp; $ -0.105 $ &amp; $ 0.066 $ \\ $12.0-15.0 $ &amp; $ 0.038 $ &amp; $ -0.011 $ &amp; $ -0.044 $ &amp; $ 0.032 $ \\ $15.0-30.0 $ &amp; $ 0.0023 $ &amp; $ -0.0009 $ &amp; $ -0.0030 $ &amp; $ 0.0015 $ \\ \hline \multicolumn{5}{c}{$2.1 < |y| < 2.4 $} \\ \hline $5.5-8.0 $ &amp; $ -0.98 $ &amp; $ 1.65 $ &amp; $ -1.65 $ &amp; $ 3.36 $ \\ $8.0-9.0 $ &amp; $ -0.20 $ &amp; $ 0.58 $ &amp; $ -0.67 $ &amp; $ 0.76 $ \\ $9.0-10.0 $ &amp; $ -0.10 $ &amp; $ 0.21 $ &amp; $ -0.27 $ &amp; $ 0.31 $ \\ $10.0-12.0 $ &amp; $ -0.060 $ &amp; $ 0.124 $ &amp; $ -0.163 $ &amp; $ 0.096 $ \\ $12.0-15.0 $ &amp; $ -0.002 $ &amp; $ 0.020 $ &amp; $ -0.022 $ &amp; $ 0.019 $ \\ $15.0-30.0 $ &amp; $ -0.0009 $ &amp; $ 0.0003 $ &amp; $ -0.0023 $ &amp; $ 0.0011 $ \\ \hline \end{tabular} \end{table}

Prompt psi(2S)

 \begin{table}[h!] \begin{tabular}{lcccc} \hline $p_T$ (GeV/$c$) &amp; $\Delta \sigma {\rm (CS_L)}$ &amp; $\Delta \sigma {\rm (CS_T)}$ &amp; $\Delta \sigma {\rm (HX_L)}$ &amp; $\Delta \sigma {\rm (HX_T)}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 1.2 $} \\ \hline $6.5-8.0 $ &amp; $ -0.007 $ &amp; $ 0.006 $ &amp; $ -0.046 $ &amp; $ 0.050 $ \\ $8.0-9.0 $ &amp; $ 0.0112 $ &amp; $ -0.0035 $ &amp; $ -0.0262 $ &amp; $ 0.0245 $ \\ $9.0-10.0 $ &amp; $ 0.0125 $ &amp; $ -0.0047 $ &amp; $ -0.0182 $ &amp; $ 0.0163 $ \\ $10.0-11.0 $ &amp; $ 0.0080 $ &amp; $ -0.0032 $ &amp; $ -0.0108 $ &amp; $ 0.0095 $ \\ $11.0-12.0 $ &amp; $ 0.0049 $ &amp; $ -0.0019 $ &amp; $ -0.0062 $ &amp; $ 0.0057 $ \\ $12.0-13.5 $ &amp; $ 0.0030 $ &amp; $ -0.0011 $ &amp; $ -0.0039 $ &amp; $ 0.0033 $ \\ $13.5-15.0 $ &amp; $ 0.00171 $ &amp; $ -0.00056 $ &amp; $ -0.00203 $ &amp; $ 0.00169 $ \\ $15.0-18.0 $ &amp; $ 0.00065 $ &amp; $ -0.00025 $ &amp; $ -0.00089 $ &amp; $ 0.00069 $ \\ $18.0-30.0 $ &amp; $ 0.000096 $ &amp; $ -0.000037 $ &amp; $ -0.000133 $ &amp; $ 0.000097 $ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $5.5-6.5 $ &amp; $ -0.185 $ &amp; $ 0.150 $ &amp; $ -0.196 $ &amp; $ 0.177 $ \\ $6.5-8.0 $ &amp; $ -0.029 $ &amp; $ 0.022 $ &amp; $ -0.056 $ &amp; $ 0.056 $ \\ $8.0-9.0 $ &amp; $ 0.0076 $ &amp; $ -0.0032 $ &amp; $ -0.0228 $ &amp; $ 0.0211 $ \\ $9.0-10.0 $ &amp; $ 0.0085 $ &amp; $ -0.0032 $ &amp; $ -0.0163 $ &amp; $ 0.0145 $ \\ $10.0-12.0 $ &amp; $ 0.0047 $ &amp; $ -0.0020 $ &amp; $ -0.0073 $ &amp; $ 0.0064 $ \\ $12.0-15.0 $ &amp; $ 0.0018 $ &amp; $ -0.0007 $ &amp; $ -0.0027 $ &amp; $ 0.0023 $ \\ $15.0-30.0 $ &amp; $ 0.00018 $ &amp; $ -0.00008 $ &amp; $ -0.00027 $ &amp; $ 0.00019 $ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.4 $} \\ \hline $5.5-6.5 $ &amp; $ -0.122 $ &amp; $ 0.130 $ &amp; $ -0.157 $ &amp; $ 0.157 $ \\ $6.5-8.0 $ &amp; $ -0.016 $ &amp; $ 0.021 $ &amp; $ -0.063 $ &amp; $ 0.053 $ \\ $8.0-9.0 $ &amp; $ 0.0026 $ &amp; $ 0.0029 $ &amp; $ -0.0260 $ &amp; $ 0.0235 $ \\ $9.0-10.0 $ &amp; $ 0.0047 $ &amp; $ 0.0014 $ &amp; $ -0.0154 $ &amp; $ 0.0143 $ \\ $10.0-12.0 $ &amp; $ 0.0028 $ &amp; $ -0.0006 $ &amp; $ -0.0065 $ &amp; $ 0.0052 $ \\ $12.0-15.0 $ &amp; $ 0.00110 $ &amp; $ -0.00026 $ &amp; $ -0.00243 $ &amp; $ 0.00177 $ \\ $15.0-30.0 $ &amp; $ 0.000100 $ &amp; $ -0.000031 $ &amp; $ -0.000210 $ &amp; $ 0.000143 $ \\ \hline \end{tabular} \end{table}

Topic attachments
I Attachment History Action Size Date Who Comment
PDFpdf 2D_ALLtimefitJpsi_pT8-9_y0-09_Log.pdf r2 r1 manage 24.7 K 2011-11-23 - 10:20 RobertoCovarelli Projection of a J/ψ two-dimensional fit on the lJ/ψ dimension in the bin: |y| < 0.9, 8.0 < pT < 9.0 GeV/c. The plot below show the distribution of the pulls.
PDFpdf 2D_ALLtimefitPsip_pT12-15_y16-24_Log.pdf r2 r1 manage 24.3 K 2011-11-23 - 10:20 RobertoCovarelli Projection of a J/ψ-ψ(2S) two-dimensional fit on the lψ(2S) dimension in the bin: 1.6 < |y| < 2.4, 12.0 < pT < 15.0 GeV/c. The plots below the distributions show the fit pulls.
PDFpdf ALLmassfitJpsi_pT12-15_y09-12.pdf r2 r1 manage 19.4 K 2011-11-23 - 10:21 RobertoCovarelli J/ψ mass distribution fit in the bin: 0.9 < |y| < 1.2, 12.0 < pT < 15.0 GeV/c.
PDFpdf ALLmassfitPsip_pT8-9_y0-12.pdf r2 r1 manage 26.4 K 2011-11-23 - 10:21 RobertoCovarelli J/ψ and ψ(2S) mass distribution fit in the bin: |y| < 1.2, 8.0 < pT < 9.0 GeV/c.
PDFpdf BRatio_av.pdf r1 manage 16.7 K 2011-11-23 - 10:40 RobertoCovarelli Measured value of the psi(2S) to J/psi differential cross-section ratio, for prompt (left) and non-prompt (right) production, averaged over rapidity and plotted as a function of pT. The left plot also includes the comparison with the NRQCD prediction, while the right plot shows the predictions of the theoretical models used to determine BR(B -> psi(2S) X), after the latter have been rescaled to the fitted value given in Eq.~(12). The shaded bands show the uncertainties on the theoretical predictions. The error bars give the total uncertainties on the measurements; polarization uncertainties are not included.
PDFpdf PRatio_av.pdf r1 manage 15.3 K 2011-11-23 - 10:39 RobertoCovarelli Measured value of the psi(2S) to J/psi differential cross-section ratio, for prompt (left) and non-prompt (right) production, averaged over rapidity and plotted as a function of pT. The left plot also includes the comparison with the NRQCD prediction, while the right plot shows the predictions of the theoretical models used to determine BR(B -> psi(2S) X), after the latter have been rescaled to the fitted value given in Eq.~(12). The shaded bands show the uncertainties on the theoretical predictions. The error bars give the total uncertainties on the measurements; polarization uncertainties are not included.
PDFpdf XS_all_alsoOld_sg_jpsi.pdf r2 r1 manage 19.7 K 2011-11-23 - 10:24 RobertoCovarelli Measured differential cross section for J/ψ inclusive production as a function of pT for five rapidity bins, plotted with the results published in [4], which extend to a lower pT range. (multiplicative factors - showing as additive offsets in log scale - are used to achieve a convenient graphical separation of the measurements from different rapidity bins.)
PDFpdf XS_all_b_sg_jpsi_teor.pdf r2 r1 manage 27.5 K 2011-11-23 - 10:25 RobertoCovarelli Measured differential cross section for non-prompt J/ψ (left) and ψ(2S) (right) pro- duction as a function of pT for the different rapidity bins. The yellow and blue coloured his- tograms indicate the theoretical predictions from FONLL calculations, the lines are added only for illustrative purposes.
PDFpdf XS_all_b_sg_noAcc_jpsi.pdf r1 manage 18.1 K 2011-11-23 - 10:35 RobertoCovarelli Measured differential cross section for non-prompt J/psi (left) and psi(2S) (right) production as a function of pT for the different rapidity bins. The error bars on data points include all the statistical and systematic contributions except luminosity. The measurements have been offset by the numerical values given in the legend for easier viewing. The result is not corrected for the muon acceptance.
PDFpdf XS_all_b_sg_noAcc_psi2s.pdf r1 manage 16.2 K 2011-11-23 - 10:36 RobertoCovarelli Measured differential cross section for non-prompt J/psi (left) and psi(2S) (right) production as a function of pT for the different rapidity bins. The error bars on data points include all the statistical and systematic contributions except luminosity. The measurements have been offset by the numerical values given in the legend for easier viewing. The result is not corrected for the muon acceptance.
PDFpdf XS_all_b_sg_psi2s_teor.pdf r3 r2 r1 manage 18.5 K 2011-11-23 - 10:59 RobertoCovarelli Measured differential cross section for non-prompt ψ(2S) (right) production as a function of pT for the different rapidity bins. The yellow and blue coloured histograms indicate the theoretical predictions from FONLL calculations, the lines are added only for illustrative purposes.
PDFpdf XS_all_p_sg_jpsi_teor.pdf r2 r1 manage 28.1 K 2011-11-23 - 10:26 RobertoCovarelli Measured differential cross section for prompt J/ψ production as a function of pT for the different rapidity bins. The yellow and blue coloured histograms indicate the theoretical predictions from NRQCD calculations, the lines are added only for illustrative purposes.
PDFpdf XS_all_p_sg_noAcc_jpsi.pdf r1 manage 18.1 K 2011-11-23 - 10:32 RobertoCovarelli Measured differential cross section for prompt J/psi (left) and psi(2S) (right) production as a function of pT for the different rapidity bins. The error bars on data points include all the statistical and systematic contributions except luminosity. The measurements have been offset by the numerical values given in the legend for easier viewing. The results are not corrected for the muon acceptance.
PDFpdf XS_all_p_sg_noAcc_psi2s.pdf r1 manage 16.2 K 2011-11-23 - 10:34 RobertoCovarelli Measured differential cross section for prompt J/psi (left) and psi(2S) (right) production as a function of pT for the different rapidity bins. The error bars on data points include all the statistical and systematic contributions except luminosity. The measurements have been offset by the numerical values given in the legend for easier viewing. The results are not corrected for the muon acceptance.
PDFpdf XS_all_p_sg_psi2s_teor.pdf r2 r1 manage 18.5 K 2011-11-23 - 10:27 RobertoCovarelli Measured differential cross section for prompt ψ(2S) production as a function of pT for the different rapidity bins. The yellow and blue coloured histograms indicate the theoretical predictions from NRQCD calculations, the lines are added only for illustrative purposes.
PDFpdf bfrac_0-12.pdf r2 r1 manage 15.2 K 2011-11-23 - 10:27 RobertoCovarelli Fitted J/ψ and ψ(2S) b-fractions plotted as a function of pT for three rapidity regions: 0 < |y| < 1.2 (top); 1.2 < |y| < 1.6 (middle); 1.6 < |y| < 2.4 (bottom). Fixed offsets have been added to some sets of points for illustrative purposes.
PDFpdf bfrac_12-16.pdf r2 r1 manage 14.5 K 2011-11-23 - 10:28 RobertoCovarelli Fitted J/ψ and ψ(2S) b-fractions plotted as a function of pT for three rapidity regions: 0 < |y| < 1.2 (top); 1.2 < |y| < 1.6 (middle); 1.6 < |y| < 2.4 (bottom). Fixed offsets have been added to some sets of points for illustrative purposes.
PDFpdf bfrac_16-24.pdf r2 r1 manage 15.7 K 2011-11-23 - 10:28 RobertoCovarelli Fitted J/ψ and ψ(2S) b-fractions plotted as a function of pT for three rapidity regions: 0 < |y| < 1.2 (top); 1.2 < |y| < 1.6 (middle); 1.6 < |y| < 2.4 (bottom). Fixed offsets have been added to some sets of points for illustrative purposes.
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Topic revision: r16 - 2014-11-12 - NunoLeonardo
 
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