The differential crosssection for the inclusive production of psi(2S) mesons in pp collisions at sqrt(s)=7 TeV has been measured with the LHCb detector. The data sample corresponds to an integrated luminosity of 36 pb1. The psi(2S) mesons are reconstructed in the decay channels psi(2S) > mu+ mu and psi(2S) > J/psi pi+ pi, with the J/psi meson decaying into two muons. Results are presented both for promptly produced psi(2S) mesons and for those originating from bhadron decays. In the kinematic range pT(psi(2S)) <= 16 GeV/c and 2 < y(psi(2S)) <= 4.5 we measure 1.44 + 0.01 + 0.12+0.20.4 mub for prompt psi(2S) production and 0.25 + 0.01 + 0.02 mub for psi(2S) from bhadron decays, where the last uncertainty on the prompt crosssection is due to the unknown psi(2S) polarization. Recent QCD calculations are found to be in good agreement with our measurements. Combining the present result with the LHCb J/psi measurements we determine the inclusive branching fraction B(b > psi(2S) X) = (2.73 + 0.06 + 0.16 + 0.24) x 10^(3), where the last uncertainty is due to the B(b > J/psi X), B(J/psi > mu+ mu) and B(psi(2S) > e+ e) branching fraction uncertainties. All above results are corrected by an erratum included as an appendix.
Invariant mass distribution for all $\psi(2S)$ candidates passing the selection cuts for the $\mu^+ \mu^$ decay (a) and the $ J\mskip 3mu/\mskip 2mu\psi\mskip 2mu(\mu^+ \mu^) \pi^+ \pi^$ decay (b). 
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Total efficiency { vs.} $ p_{\mathrm{T}}$ computed from simulation for unpolarized $\psi {(2S)}$ mesons for $\psi(2S) \rightarrow \mu^+\mu^$ (a) and $\psi(2S) \rightarrow J\mskip 3mu/\mskip 2mu\psi\mskip 2mu(\mu^+ \mu^) \pi^+ \pi^$ (b). 
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Pseudodecaytime distribution for $\psi(2S) \rightarrow \mu^+ \mu^ $ (a) and $\psi(2S) \rightarrow J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \pi^+ \pi^ $(b) in the $ p_{\mathrm{T}}$ range $4< p_{\mathrm{T}} \le5$ $\text{ Ge V /}c$ , showing the background and prompt contributions. 
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Fraction of prompt $\psi(2S)$ as a function of $ p_{\mathrm{T}}$ for the $\mu^+ \mu^$ mode (solid squares) and the $ J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \pi^+ \pi^$ mode (open squares). Error bars include the statistical uncertainties and the systematic uncertainties due to the fitting procedure. This figure is updated in the Erratum (Appendix A). 
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Dipion mass spectrum for the $\psi(2S) \rightarrow J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \pi^+ \pi^$ decay. The curve shows the result of the fit with Eq. (3) corrected for the acceptance. 
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Comparison of the differential crosssections measured for prompt $\psi(2S)$ (circles) and for $\psi(2S)$ from $b$hadron decay (squares) in the $\psi(2S) \rightarrow \mu^+ \mu^$ (solid symbols) and $\psi(2S) \rightarrow J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \pi^+ \pi^$ (open symbols) modes. Only the uncorrelated uncertainties are shown. \bf{This figure is obsolete. Corrected cross sections are found in Figs. 7 and 8 in the Erratum}. 
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Differential production crosssection { vs.} $ p_{\mathrm{T}}$ for prompt $\psi(2S)$. The predictions of three nonrelativistic QCD models are also shown for comparison. MWC \cite{bib:chao} and KB \cite{bib:bernd} are NLO calculations including coloursinglet and colouroctet contributions. AL \cite{bib:Lansberg,bib:Lansberg2} is a coloursinglet model including the dominant NNLO terms. This figure is updated in the Erratum. 
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Differential production crosssection { vs.} $ p_{\mathrm{T}}$ for $\psi(2S)$ from $b$hadrons. The shaded band is the prediction of a FONLL calculation \cite{bib:FONLL_1,bib:FONLL_2,bib:cacciari}. This figure is updated in the Erratum. 
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Ratio of $\psi(2S) \rightarrow \mu^+ \mu^$ to $ J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \rightarrow \mu^+ \mu^$ crosssections for prompt % production (a) and for $b$hadron decay (b), as a function of $ p_{\mathrm{T}}$ . This figure is updated in the Erratum. 
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Fraction of prompt $\psi {(2S)}$ , $f_\mathrm{p}$, as a function of $ p_{\mathrm{T}}$ . The error bars include statistical and systematic uncertainties added in quadrature. 
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Differential production crosssection of prompt $\psi {(2S)}$ as a function of $ p_{\mathrm{T}}$ in the range $2.0 < y < 4.5$. The results are compared with the NRQCD calculations \cite{Shao:2014yta}. The error bars include statistical and systematic uncertainties added in quadrature. 
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Differential production crosssection of $\psi {(2S)}$ from $b$ hadrons as a function of $ p_{\mathrm{T}}$ in the range $2.0 < y < 4.5$. The results are compared with the FONLL calculations \cite{Cacciari:1998it}. The error bars include statistical and systematic uncertainties added in quadrature. 
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Ratio of $\psi {(2S)} \rightarrow \mu^+ \mu^$ and $ J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \rightarrow \mu ^+\mu ^ $ crosssections for prompt production (a) and for bhadron decay (b), as a fucntion of $ p_{\mathrm{T}}$ . 
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Animated gif made out of all figures. 
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Systematic uncertainties included in the measurement of the crosssection. Uncertainties labelled with $a$ are correlated between the $\mu^+ \mu^$ and $ J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \pi^+ \pi^$ mode, while $b$ indicates a correlation between $\psi(2S) \rightarrow \mu^+ \mu^$ and the $ J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \rightarrow \mu^+ \mu^$ uncertainties \cite{bib:jpsi}. 
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Crosssection values for prompt $\psi(2S)$ and $\psi(2S)$ from $b$hadrons in different $ p_{\mathrm{T}}$ bins and in the range $2 < y \le 4.5$, evaluated as the weighted average of the $\mu^+ \mu^$ and $ J\mskip 3mu/\mskip 2mu\psi\mskip 2mu \pi^+ \pi^$ channels. The first error is statistical, the second error is systematic, and the last asymmetric uncertainty is due to the unknown polarization of the prompt $\psi(2S)$ meson. This table is updated in the Erratum. 
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Differential crosssections $\mathrm{d}\sigma/\mathrm{d} p_{\mathrm{T}} $ (in $\text{ nb}$ /( $ {\mathrm{Ge V /}c}$ )) of prompt $\psi {(2S)}$ and $\psi {(2S)}$ from$b$ hadrons at $\sqrt{s} = 7\text{ Te V} $, integrated over $y$ between 2.0 and 4.5. The first uncertainty is statistical and the second systematic. The third asymmetric uncertainty for the prompt $\psi {(2S)}$ mesons is due to the unknown polarisation. 
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Created on 22 October 2019.