cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77015.v1/t14
title: "Table 14" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.77015.v1/t8
title: "Table 8" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality, at forward rapidity, 1.6$&lt;|y|&lt;$2.4, for two different $p_{\rm T}$ regions.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.77015.v1/t9
title: "Table 9" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nonprompt J/$\psi$ $v_{2}$ as a function of $p_{\rm T}$.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.63972.v1/t10
title: "Table 10" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t11
title: "Table 11" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t3
title: "Table 3" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t4
title: "Table 4" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t5
title: "Table 5" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t6
title: "Table 6" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t7
title: "Table 7" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t8
title: "Table 8" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t9
title: "Table 9" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t12
title: "Table 12" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t13
title: "Table 13" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t14
title: "Table 14" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t15
title: "Table 15" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t16
title: "Table 16" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t17
title: "Table 17" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t18
title: "Table 18" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t19
title: "Table 19" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t20
title: "Table 20" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t21
title: "Table 21" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t22
title: "Table 22" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t23
title: "Table 23" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t24
title: "Table 24" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t27
title: "Table 27" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.63972.v1/t25
title: "Table 25" of "Study of the production of charged pions, kaons, and protons in pPb collisions at sqrt(sNN) = 5.02 TeV"

description: .
description: CERN-LHC. Spectra of identified charged hadrons are measured in pPb collisions with the CMS detector at the LHC at sqrt(sNN) = 5.02 TeV using data taken in September 2012. Charged pions, kaons, and protons in the transverse-momentum range pT approximately 0.1-1.7 GeV and laboratory rapidity |y| &lt; 1 are identified via their energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the form: 
 d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n 
 where C=(n-1)(n-2)/(nT(nT+(n-2)m)) and mt=sqrt(m**2+pt**2). 
Tables of the fitted dN/dy, n and T are given at the end of the record.