cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.63972.v1/t26
title: "Table 26" 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/t28
title: "Table 28" 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/t29
title: "Table 29" 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/t30
title: "Table 30" 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/t31
title: "Table 31" 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/t32
title: "Table 32" 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/t33
title: "Table 33" 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/t34
title: "Table 34" 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/t35
title: "Table 35" 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/t36
title: "Table 36" 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/t37
title: "Table 37" 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/t38
title: "Table 38" 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/t39
title: "Table 39" 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/t40
title: "Table 40" 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/t41
title: "Table 41" 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/t42
title: "Table 42" 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/t43
title: "Table 43" 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/t44
title: "Table 44" 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/t45
title: "Table 45" 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/t46
title: "Table 46" 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.66784.v1/t1
title: "Table 1" of "Long-range two-particle correlations of strange hadrons with charged particles in pPb and PbPb collisions at LHC energies"

description: The elliptic flow v2(2, $|\Delta\eta| &gt; 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the $N_{offline}^{trk}$ &lt; 35 multiplicity class in pPb.
description: CERN-LHC. Measurements of two-particle angular correlations between an identified strange hadron (K0S or Lambda/anti-Lambda) and a charged particle, emitted in pPb collisions, are presented over a wide range in pseudorapidity and full azimuth. The data, corresponding to an integrated luminosity of approximately 35 inverse nanobarns, were collected at a nucleon-nucleon center-of-mass energy (sqrt(s[NN])) of 5.02 TeV with the CMS detector at the LHC. The results are compared to semi-peripheral PbPb collision data at sqrt(s[NN]) = 2.76 TeV, covering similar charged-particle multiplicities in the events. The observed azimuthal correlations at large relative pseudorapidity are used to extract the second-order (v[2]) and third-order (v[3]) anisotropy harmonics of K0S and Lambda/anti-Lambda particles. These quantities are studied as a function of the charged-particle multiplicity in the event and the transverse momentum of the particles. For high-multiplicity pPb events, a clear particle species dependence of v[2] and v[3] is observed. For pt &lt; 2 GeV, the v[2] and v[3] values of K0S particles are larger than those of Lambda/anti-Lambda particles at the same pt. This splitting effect between two particle species is found to be stronger in pPb than in PbPb collisions in the same multiplicity range. When divided by the number of constituent quarks and compared at the same transverse kinetic energy per quark, both v[2] and v[3] for K0S particles are observed to be consistent with those for Lambda/anti-Lambda particles at the 10% level in pPb collisions. This consistency extends over a wide range of particle transverse kinetic energy and event multiplicities.
DOI: 10.17182/hepdata.66784.v1/t2
title: "Table 2" of "Long-range two-particle correlations of strange hadrons with charged particles in pPb and PbPb collisions at LHC energies"

description: The elliptic flow v2(2, $|\Delta\eta| &gt; 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 35 $\leq N_{offline}^{trk}$ &lt; 60 multiplicity class in pPb.
description: CERN-LHC. Measurements of two-particle angular correlations between an identified strange hadron (K0S or Lambda/anti-Lambda) and a charged particle, emitted in pPb collisions, are presented over a wide range in pseudorapidity and full azimuth. The data, corresponding to an integrated luminosity of approximately 35 inverse nanobarns, were collected at a nucleon-nucleon center-of-mass energy (sqrt(s[NN])) of 5.02 TeV with the CMS detector at the LHC. The results are compared to semi-peripheral PbPb collision data at sqrt(s[NN]) = 2.76 TeV, covering similar charged-particle multiplicities in the events. The observed azimuthal correlations at large relative pseudorapidity are used to extract the second-order (v[2]) and third-order (v[3]) anisotropy harmonics of K0S and Lambda/anti-Lambda particles. These quantities are studied as a function of the charged-particle multiplicity in the event and the transverse momentum of the particles. For high-multiplicity pPb events, a clear particle species dependence of v[2] and v[3] is observed. For pt &lt; 2 GeV, the v[2] and v[3] values of K0S particles are larger than those of Lambda/anti-Lambda particles at the same pt. This splitting effect between two particle species is found to be stronger in pPb than in PbPb collisions in the same multiplicity range. When divided by the number of constituent quarks and compared at the same transverse kinetic energy per quark, both v[2] and v[3] for K0S particles are observed to be consistent with those for Lambda/anti-Lambda particles at the 10% level in pPb collisions. This consistency extends over a wide range of particle transverse kinetic energy and event multiplicities.
DOI: 10.17182/hepdata.66784.v1/t3
title: "Table 3" of "Long-range two-particle correlations of strange hadrons with charged particles in pPb and PbPb collisions at LHC energies"

description: The elliptic flow v2(2, $|\Delta\eta| &gt; 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 60 $\leq N_{offline}^{trk}$ &lt; 120 multiplicity class in pPb.
description: CERN-LHC. Measurements of two-particle angular correlations between an identified strange hadron (K0S or Lambda/anti-Lambda) and a charged particle, emitted in pPb collisions, are presented over a wide range in pseudorapidity and full azimuth. The data, corresponding to an integrated luminosity of approximately 35 inverse nanobarns, were collected at a nucleon-nucleon center-of-mass energy (sqrt(s[NN])) of 5.02 TeV with the CMS detector at the LHC. The results are compared to semi-peripheral PbPb collision data at sqrt(s[NN]) = 2.76 TeV, covering similar charged-particle multiplicities in the events. The observed azimuthal correlations at large relative pseudorapidity are used to extract the second-order (v[2]) and third-order (v[3]) anisotropy harmonics of K0S and Lambda/anti-Lambda particles. These quantities are studied as a function of the charged-particle multiplicity in the event and the transverse momentum of the particles. For high-multiplicity pPb events, a clear particle species dependence of v[2] and v[3] is observed. For pt &lt; 2 GeV, the v[2] and v[3] values of K0S particles are larger than those of Lambda/anti-Lambda particles at the same pt. This splitting effect between two particle species is found to be stronger in pPb than in PbPb collisions in the same multiplicity range. When divided by the number of constituent quarks and compared at the same transverse kinetic energy per quark, both v[2] and v[3] for K0S particles are observed to be consistent with those for Lambda/anti-Lambda particles at the 10% level in pPb collisions. This consistency extends over a wide range of particle transverse kinetic energy and event multiplicities.