CMSPublic Web>PhysicsResults>PhysicsResultsBPH>PhysicsResultsBPH10014 (2014-11-12, NunoLeonardo)

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

Non Prompt

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

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

Prompt

Non Prompt

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

Prompt

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

Non Prompt

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

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

and the J/psi criteria:

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

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

Prompt

Non Prompt

Cross section ratios

Prompt

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

Non prompt

$\begin{table}[htdp] \begin{tabular}{lccc} \hline $p_T~({\rm GeV}/c)$ & $\frac{\frac{d^2\sigma}{dp_\mathrm{T}dy}(\psi{\rm (2S)}) \cdot \mbox{BR}(\psi{\rm (2S)} \rightarrow \mu^{+}\mu^{-})}{\frac{d^2\sigma}{dp_\mathrm{T}dy}(J/\psi) \cdot \mbox{BR}(J/\psi \rightarrow \mu^{+}\mu^{-})}$ & $\pm \sigma_{\rm stat}$ & $\pm \sigma_{\rm syst}$ \\ \hline \multicolumn{4}{c}{$|y| < 1.2$} \\ \hline $8-9$ & $0.0480 $ & $ 0.0022 $ & $ 0.0028 $ \\ $9-10$ & $0.0483 $ & $ 0.0019 $ & $ 0.0024 $ \\ $10-11$ & $0.0452 $ & $ 0.0019 $ & $ 0.0020 $ \\ $11-12$ & $0.0466 $ & $ 0.0021 $ & $ 0.0019 $ \\ $12-13$ & $0.0519 $ & $ 0.0021 $ & $ 0.0023 $ \\ $13-15$ & $0.0527 $ & $ 0.0025 $ & $ 0.0021 $ \\ $15-18$ & $0.0475 $ & $ 0.0022 $ & $ 0.0019 $ \\ $18-30$ & $0.054 $ & $ 0.002 $ & $ 0.003 $ \\ \hline \multicolumn{4}{c}{$1.2 < |y| < 1.6$} \\ \hline $6.5-8$ & $0.054 $ & $ 0.003 $ & $ 0.008 $ \\ $8-9$ & $0.042 $ & $ 0.003 $ & $ 0.006 $ \\ $9-10$ & $0.047 $ & $ 0.004 $ & $ 0.007 $ \\ $10-12$ & $0.047 $ & $ 0.003 $ & $ 0.007 $ \\ $12-15$ & $0.049 $ & $ 0.005 $ & $ 0.009 $ \\ $15-30$ & $0.063 $ & $ 0.003 $ & $ 0.009 $ \\ \hline \multicolumn{4}{c}{$1.6 < |y| < 2.4$} \\ \hline $6.5-8$ & $0.0318 $ & $ 0.0023 $ & $ 0.0029 $ \\ $8-9$ & $0.0435 $ & $ 0.0034 $ & $ 0.0027 $ \\ $9-10$ & $0.042 $ & $ 0.004 $ & $ 0.004 $ \\ $10-12$ & $0.0468 $ & $ 0.0034 $ & $ 0.0029 $ \\ $12-15$ & $0.0446 $ & $ 0.0031 $ & $ 0.0025 $ \\ $15-30$ & $0.0451 $ & $ 0.0039 $ & $ 0.0021 $ \\ \hline \multicolumn{4}{c}{Integrated: $|y| < 2.4$} \\ \hline $6.5-8$ & $0.0390 $ & $ 0.0031 $ & $ 0.0052 $ \\ $8-9$ & $0.0455 $ & $ 0.0026 $ & $ 0.0033 $ \\ $9-10$ & $0.0470 $ & $ 0.0032 $ & $ 0.0034 $ \\ $10-12$ & $0.0460 $ & $ 0.0022 $ & $ 0.0033 $ \\ $12-15$ & $0.0504 $ & $ 0.0022 $ & $ 0.0033 $ \\ $15-30$ & $0.0499 $ & $ 0.0020 $ & $ 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 $|y|$ & $p_T~({\rm GeV}/c)$ & $f_B(J/\psi)$ \\ \hline $0.0-0.9$ & $8.0-9.0$ & $0.271 \pm 0.006 \pm 0.003$ \\ & $9.0-10.0$ & $0.285 \pm 0.005 \pm 0.004$ \\ & $10.0-11.0$ & $0.320 \pm 0.005 \pm 0.004$ \\ & $11.0-12.0$ & $0.345 \pm 0.005 \pm 0.007$ \\ & $12.0-13.5$ & $0.373 \pm 0.005 \pm 0.003$ \\ & $13.5-15.0$ & $0.417 \pm 0.006 \pm 0.005$ \\ & $15.0-18.0$ & $0.454 \pm 0.006 \pm 0.004$ \\ & $18.0-30.0$ & $0.535 \pm 0.006 \pm 0.004$ \\ & $30.0-45.0$ & $0.633 \pm 0.015 \pm 0.010$ \\ & $45.0-70.0$ & $0.646 \pm 0.038 \pm 0.024$ \\ \hline $0.9-1.2$ & $8.0-9.0$ & $0.265 \pm 0.007 \pm 0.007$ \\ & $9.0-10.0$ & $0.281 \pm 0.007 \pm 0.007$ \\ & $10.0-12.0$ & $0.324 \pm 0.006 \pm 0.007$ \\ & $12.0-15.0$ & $0.380 \pm 0.006 \pm 0.008$ \\ & $15.0-30.0$ & $0.481 \pm 0.007 \pm 0.007$ \\ & $30.0-45.0$ & $0.616 \pm 0.029 \pm 0.028$ \\ \hline $1.2-1.6$ & $6.5-7.0$ & $0.207 \pm 0.010 \pm 0.006$ \\ & $7.0-7.5$ & $0.221 \pm 0.009 \pm 0.006$ \\ & $7.5-8.0$ & $0.219 \pm 0.007 \pm 0.012$ \\ & $8.0-8.5$ & $0.238 \pm 0.007 \pm 0.011$ \\ & $8.5-9.0$ & $0.253 \pm 0.007 \pm 0.009$ \\ & $9.0-10.0$ & $0.275 \pm 0.006 \pm 0.008$ \\ & $10.0-11.0$ & $0.299 \pm 0.006 \pm 0.009$ \\ & $11.0-12.0$ & $0.335 \pm 0.007 \pm 0.009$ \\ & $12.0-15.0$ & $0.376 \pm 0.006 \pm 0.011$ \\ & $15.0-30.0$ & $0.466 \pm 0.007 \pm 0.013$ \\ & $30.0-45.0$ & $0.583 \pm 0.026 \pm 0.024$ \\ \hline $1.6-2.1$ & $6.50-7.00$ & $0.199 \pm 0.010 \pm 0.012$ \\ & $7.00-7.25$ & $0.225 \pm 0.013 \pm 0.010$ \\ & $7.25-7.50$ & $0.239 \pm 0.013 \pm 0.010$ \\ & $7.50-8.00$ & $0.233 \pm 0.009 \pm 0.013$ \\ & $8.00-8.50$ & $0.237 \pm 0.009 \pm 0.015$ \\ & $8.50-9.00$ & $0.250 \pm 0.009 \pm 0.014$ \\ & $9.00-10.00$ & $0.258 \pm 0.007 \pm 0.014$ \\ & $10.00-11.00$ & $0.299 \pm 0.008 \pm 0.010$ \\ & $11.00-12.00$ & $0.321 \pm 0.010 \pm 0.015$ \\ & $12.00-15.00$ & $0.356 \pm 0.008 \pm 0.017$ \\ & $15.00-30.00$ & $0.458 \pm 0.009 \pm 0.019$ \\ \hline $2.1-2.4$ & $5.5-8.0$ & $0.214 \pm 0.012 \pm 0.013$ \\ & $8.0-9.0$ & $0.226 \pm 0.016 \pm 0.020$ \\ & $9.0-10.0$ & $0.275 \pm 0.018 \pm 0.020$ \\ & $10.0-12.0$ & $0.294 \pm 0.014 \pm 0.018$ \\ & $12.0-15.0$ & $0.368 \pm 0.016 \pm 0.017$ \\ & $15.0-30.0$ & $0.432 \pm 0.020 \pm 0.023$ \\ \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 $|y|$ & $p_T$ (GeV/$c$) & $f_B(\psi{\rm (2S)})$ & $f_B(\psi{\rm (2S)})/f_B(J/\psi)$ \\ \hline $0.0-1.2$ & $6.5-8.0$ & $0.326 \pm 0.041 \pm 0.011$ & $1.46 \pm 0.19 \pm 0.08$ \\ & $8.0-9.0$ & $0.350 \pm 0.025 \pm 0.014$ & $1.30 \pm 0.12 \pm 0.08$ \\ & $9.0-10.0$ & $0.335 \pm 0.021 \pm 0.020$ & $1.20 \pm 0.08 \pm 0.08$ \\ & $10.0-11.0$ & $0.378 \pm 0.023 \pm 0.022$ & $1.19 \pm 0.08 \pm 0.07$ \\ & $11.0-12.0$ & $0.394 \pm 0.024 \pm 0.028$ & $1.16 \pm 0.07 \pm 0.09$ \\ & $12.0-13.5$ & $0.431 \pm 0.022 \pm 0.020$ & $1.16 \pm 0.06 \pm 0.05$ \\ & $13.5-15.0$ & $0.456 \pm 0.025 \pm 0.028$ & $1.10 \pm 0.06 \pm 0.07$ \\ & $15.0-18.0$ & $0.487 \pm 0.024 \pm 0.017$ & $1.08 \pm 0.05 \pm 0.04$ \\ & $18.0-30.0$ & $0.572 \pm 0.025 \pm 0.028$ & $1.08 \pm 0.05 \pm 0.05$ \\ \hline $1.2-1.6$ & $5.5-6.5$ & $0.246 \pm 0.093 \pm 0.029$ & $1.33 \pm 0.51 \pm 0.22$ \\ & $6.5-8.0$ & $0.308 \pm 0.030 \pm 0.010$ & $1.42 \pm 0.14 \pm 0.07$ \\ & $8.0-9.0$ & $0.309 \pm 0.035 \pm 0.022$ & $1.26 \pm 0.14 \pm 0.11$ \\ & $9.0-10.0$ & $0.32 \pm 0.03 \pm 0.04$ & $1.18 \pm 0.12 \pm 0.14$ \\ & $10.0-12.0$ & $0.366 \pm 0.029 \pm 0.028$ & $1.16 \pm 0.09 \pm 0.09$ \\ & $12.0-15.0$ & $0.375 \pm 0.032 \pm 0.028$ & $1.00 \pm 0.09 \pm 0.07$ \\ & $15.0-30.0$ & $0.51 \pm 0.03 \pm 0.04$ & $1.09 \pm 0.07 \pm 0.08$ \\ \hline $1.6-2.4$ & $5.5-6.5$ & $0.21 \pm 0.06 \pm 0.07$ & $1.2 \pm 0.3 \pm 0.3$ \\ & $6.5-8.0$ & $0.19 \pm 0.03 \pm 0.03$ & $0.88 \pm 0.13 \pm 0.13$ \\ & $8.0-9.0$ & $0.30 \pm 0.04 \pm 0.04$ & $1.24 \pm 0.15 \pm 0.18$ \\ & $9.0-10.0$ & $0.30 \pm 0.04 \pm 0.05$ & $1.14 \pm 0.17 \pm 0.19$ \\ & $10.0-12.0$ & $0.37 \pm 0.03 \pm 0.04$ & $1.23 \pm 0.11 \pm 0.14$ \\ & $12.0-15.0$ & $0.372 \pm 0.035 \pm 0.015$ & $1.04 \pm 0.10 \pm 0.07$ \\ & $15.0-30.0$ & $0.45 \pm 0.04 \pm 0.04$ & $0.97 \pm 0.09 \pm 0.07$ \\ \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/$c$) & $\Delta \sigma {\rm (CS_L)}$ & $\Delta \sigma {\rm (CS_T)}$ & $\Delta \sigma {\rm (HX_L)}$ & $\Delta \sigma {\rm (HX_T)}$ \\ \hline \multicolumn{5}{c}{$0 < |y| < 0.9 $} \\ \hline $8.0-9.0 $ & $ 0.21 $ & $ -0.06 $ & $ -0.62 $ & $ 0.58 $ \\ $9.0-10.0 $ & $ 0.22 $ & $ -0.06 $ & $ -0.37 $ & $ 0.31 $ \\ $10.0-11.0 $ & $ 0.155 $ & $ -0.049 $ & $ -0.213 $ & $ 0.170 $ \\ $11.0-12.0 $ & $ 0.085 $ & $ -0.031 $ & $ -0.127 $ & $ 0.087 $ \\ $12.0-13.5 $ & $ 0.037 $ & $ -0.013 $ & $ -0.065 $ & $ 0.050 $ \\ $13.5-15.0 $ & $ 0.022 $ & $ -0.008 $ & $ -0.030 $ & $ 0.020 $ \\ $15.0-18.0 $ & $ 0.0066 $ & $ -0.0027 $ & $ -0.0124 $ & $ 0.0080 $ \\ $18.0-30.0 $ & $ 0.0009 $ & $ -0.0003 $ & $ -0.0015 $ & $ 0.0008 $ \\ $30.0-45.0 $ & $ 0 $ & $ 0 $ & $ 0 $ & $ 0 $ \\ $45.0-70.0 $ & $ 0 $ & $ 0 $ & $ 0 $ & $ 0 $ \\ \hline \multicolumn{5}{c}{$0.9 < |y| < 1.2 $} \\ \hline $8.0-9.0 $ & $ 0.64 $ & $ -0.21 $ & $ -0.61 $ & $ 0.62 $ \\ $9.0-10.0 $ & $ 0.26 $ & $ -0.11 $ & $ -0.36 $ & $ 0.28 $ \\ $10.0-12.0 $ & $ 0.109 $ & $ -0.040 $ & $ -0.156 $ & $ 0.134 $ \\ $12.0-15.0 $ & $ 0.033 $ & $ -0.011 $ & $ -0.040 $ & $ 0.028 $ \\ $15.0-30.0 $ & $ 0.0019 $ & $ -0.0008 $ & $ -0.0034 $ & $ 0.0019 $ \\ $30.0-45.0 $ & $ 0 $ & $ 0 $ & $ 0 $ & $ 0 $ \\ \hline \multicolumn{5}{c}{$1.2 < |y| < 1.6 $} \\ \hline $6.5-7.0 $ & $ -1.46 $ & $ 1.06 $ & $ -1.90 $ & $ 2.13 $ \\ $7.0-7.5 $ & $ -0.56 $ & $ 0.34 $ & $ -1.25 $ & $ 1.19 $ \\ $7.5-8.0 $ & $ -0.04 $ & $ -0.03 $ & $ -1.05 $ & $ 0.71 $ \\ $8.0-8.5 $ & $ 0.19 $ & $ -0.01 $ & $ -0.70 $ & $ 0.52 $ \\ $8.5-9.0 $ & $ 0.24 $ & $ -0.06 $ & $ -0.51 $ & $ 0.38 $ \\ $9.0-10.0 $ & $ 0.18 $ & $ -0.07 $ & $ -0.33 $ & $ 0.27 $ \\ $10.0-11.0 $ & $ 0.095 $ & $ -0.030 $ & $ -0.174 $ & $ 0.138 $ \\ $11.0-12.0 $ & $ 0.048 $ & $ -0.029 $ & $ -0.104 $ & $ 0.075 $ \\ $12.0-15.0 $ & $ 0.023 $ & $ -0.008 $ & $ -0.039 $ & $ 0.025 $ \\ $15.0-30.0 $ & $ 0.0012 $ & $ -0.0007 $ & $ -0.0026 $ & $ 0.0017 $ \\ $30.0-45.0 $ & $ 0 $ & $ 0 $ & $ 0 $ & $ 0 $ \\ \hline \multicolumn{5}{c}{$1.6 < |y| < 2.1 $} \\ \hline $6.5-7.0 $ & $ -0.17 $ & $ 0.18 $ & $ -2.22 $ & $ 2.26 $ \\ $7.0-7.25 $ & $ 0.71 $ & $ 0.09 $ & $ -1.54 $ & $ 1.33 $ \\ $7.25-7.5 $ & $ 0.77 $ & $ -0.23 $ & $ -1.19 $ & $ 1.01 $ \\ $7.5-8.0 $ & $ 0.57 $ & $ -0.13 $ & $ -0.98 $ & $ 0.70 $ \\ $8.0-8.5 $ & $ 0.51 $ & $ -0.14 $ & $ -0.69 $ & $ 0.55 $ \\ $8.5-9.0 $ & $ 0.43 $ & $ -0.12 $ & $ -0.53 $ & $ 0.44 $ \\ $9.0-10.0 $ & $ 0.23 $ & $ -0.08 $ & $ -0.33 $ & $ 0.26 $ \\ $10.0-11.0 $ & $ 0.118 $ & $ -0.056 $ & $ -0.182 $ & $ 0.144 $ \\ $11.0-12.0 $ & $ 0.065 $ & $ -0.023 $ & $ -0.105 $ & $ 0.066 $ \\ $12.0-15.0 $ & $ 0.038 $ & $ -0.011 $ & $ -0.044 $ & $ 0.032 $ \\ $15.0-30.0 $ & $ 0.0023 $ & $ -0.0009 $ & $ -0.0030 $ & $ 0.0015 $ \\ \hline \multicolumn{5}{c}{$2.1 < |y| < 2.4 $} \\ \hline $5.5-8.0 $ & $ -0.98 $ & $ 1.65 $ & $ -1.65 $ & $ 3.36 $ \\ $8.0-9.0 $ & $ -0.20 $ & $ 0.58 $ & $ -0.67 $ & $ 0.76 $ \\ $9.0-10.0 $ & $ -0.10 $ & $ 0.21 $ & $ -0.27 $ & $ 0.31 $ \\ $10.0-12.0 $ & $ -0.060 $ & $ 0.124 $ & $ -0.163 $ & $ 0.096 $ \\ $12.0-15.0 $ & $ -0.002 $ & $ 0.020 $ & $ -0.022 $ & $ 0.019 $ \\ $15.0-30.0 $ & $ -0.0009 $ & $ 0.0003 $ & $ -0.0023 $ & $ 0.0011 $ \\ \hline \end{tabular} \end{table}$

Prompt psi(2S)

Attachments

Topic attachments
I	Attachment	History	Action	Size	Date	Who	Comment
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.)
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.
pdf	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.

Topic revision: r16 - 2014-11-12 - NunoLeonardo

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Measurement of the and cross section in pp collisions at √s = 7 TeV

Abstract

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

Tables of numerical results

Cross Sections

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

Prompt

Non Prompt

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

Prompt

Non Prompt

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

Prompt

Non Prompt

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

Prompt

Non Prompt

Cross section ratios

Prompt

Non prompt

Non-prompt fractions

Variations of prompt cross-sections with extreme polarization scenarios

Prompt J/psi

Prompt psi(2S)

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