cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.60488.v1/t16
title: "Table 16" of "Inelastic Production of J/psi Mesons in Photoproduction and Deep Inelastic Scattering at HERA"

description: Measured polarization parameter in the Helicity Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).
description: DESY-HERA. Measurement of the inelastic photo- and electroproduction of J/PSI mesons in E- P scattering. The data were taken from 2004 to 2007 with both electron and positron beams. For both samples the photon-proton centre of mass energy, W, is from 60 to 240 GeV and the inelasticity, Z, from 0.3 to 0.9. For the photoproduction sample the Q**2 is &lt; 2.5 GeV**2 with a mean of 0.085 GeV**2 and for the electroproduction sample Q**2 is from 3.6 to 100 GeV**2. For the photoproduction sample PT in the lab frame is &gt; 1.0 GeV and for the electroproduction sample PT is &gt; 1.0 GeV in the photon-proton rest frame. Differential cross sections are given as functions of PT, Z, W and Q**2.
DOI: 10.17182/hepdata.60488.v1/t17
title: "Table 17" of "Inelastic Production of J/psi Mesons in Photoproduction and Deep Inelastic Scattering at HERA"

description: Measured polarization parameter in the Collins-Soper Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).
description: DESY-HERA. Measurement of the inelastic photo- and electroproduction of J/PSI mesons in E- P scattering. The data were taken from 2004 to 2007 with both electron and positron beams. For both samples the photon-proton centre of mass energy, W, is from 60 to 240 GeV and the inelasticity, Z, from 0.3 to 0.9. For the photoproduction sample the Q**2 is &lt; 2.5 GeV**2 with a mean of 0.085 GeV**2 and for the electroproduction sample Q**2 is from 3.6 to 100 GeV**2. For the photoproduction sample PT in the lab frame is &gt; 1.0 GeV and for the electroproduction sample PT is &gt; 1.0 GeV in the photon-proton rest frame. Differential cross sections are given as functions of PT, Z, W and Q**2.
DOI: 10.17182/hepdata.60488.v1/t18
title: "Table 18" of "Inelastic Production of J/psi Mesons in Photoproduction and Deep Inelastic Scattering at HERA"

description: Measured polarization parameter in the Helicity Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).
description: DESY-HERA. Measurement of the inelastic photo- and electroproduction of J/PSI mesons in E- P scattering. The data were taken from 2004 to 2007 with both electron and positron beams. For both samples the photon-proton centre of mass energy, W, is from 60 to 240 GeV and the inelasticity, Z, from 0.3 to 0.9. For the photoproduction sample the Q**2 is &lt; 2.5 GeV**2 with a mean of 0.085 GeV**2 and for the electroproduction sample Q**2 is from 3.6 to 100 GeV**2. For the photoproduction sample PT in the lab frame is &gt; 1.0 GeV and for the electroproduction sample PT is &gt; 1.0 GeV in the photon-proton rest frame. Differential cross sections are given as functions of PT, Z, W and Q**2.
DOI: 10.17182/hepdata.60488.v1/t19
title: "Table 19" of "Inelastic Production of J/psi Mesons in Photoproduction and Deep Inelastic Scattering at HERA"

description: Measured polarization parameter in the Collins-Soper Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).
description: DESY-HERA. Measurement of the inelastic photo- and electroproduction of J/PSI mesons in E- P scattering. The data were taken from 2004 to 2007 with both electron and positron beams. For both samples the photon-proton centre of mass energy, W, is from 60 to 240 GeV and the inelasticity, Z, from 0.3 to 0.9. For the photoproduction sample the Q**2 is &lt; 2.5 GeV**2 with a mean of 0.085 GeV**2 and for the electroproduction sample Q**2 is from 3.6 to 100 GeV**2. For the photoproduction sample PT in the lab frame is &gt; 1.0 GeV and for the electroproduction sample PT is &gt; 1.0 GeV in the photon-proton rest frame. Differential cross sections are given as functions of PT, Z, W and Q**2.
DOI: 10.17182/hepdata.60489.v1/t1
title: "Table 1" of "Measurement of the sum of WW and WZ production with W+dijet events in pp collisions at sqrt(s) = 7 TeV"

description: Integrated cross section for inclusive WW + WZ production from the electron and muon channels combined.
description: CERN LHC. Measurement of the inclusive cross section for WW ans WZ diboson production in proton-proton collisions at a centre of mass energy of 7 TeV. The data sample used has an integrated luminosity of 5.0 fb-1.
DOI: 10.17182/hepdata.60510.v1/t1
title: "Table 1" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The centrality dependence of the three-particle charge-dependent correlator MEAN(COS(PHI(A)+COS(PHI(B)-2*PHI(RP)) measured with the cumulant method.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t2
title: "Table 2" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The centrality dependence of the correlator three-particle charge-dependent MEAN(COS(PHI(A)+COS(PHI(B)-2*PHI(RP)) measured from correlations with the reaction plane (RP) estimated using the TPC detector.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t3
title: "Table 3" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The centrality dependence of the correlator three-particle charge-dependent MEAN(COS(PHI(A)+COS(PHI(B)-2*PHI(RP)) measured from correlations with the reaction plane (RP) estimated using the VZERO detector.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t4
title: "Table 4" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The centrality dependence of the correlator three-particle charge-dependent MEAN(COS(PHI(A)+COS(PHI(B)-2*PHI(RP)) measured from correlations with the reaction plane (RP) estimated using the ZDC detector.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t5
title: "Table 5" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The centrality dependence of the two-particle charge-dependentcorrelator MEAN(COS(PHI(A)-COS(PHI(B)) measured with the cumulant method.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t10
title: "Table 10" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The dependence of the three-particle charge-dependent correlator MEAN(COS(PHI(A)+COS(PHI(B)-2*PHI(RP)) on the difference in pseudorapidity of the two particles A and B for the centrality range 30-40%.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t6
title: "Table 6" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The decomposition of the correlators into the COS*COS terms.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t7
title: "Table 7" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The decomposition of the correlators into the SIN*SIN terms.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t8
title: "Table 8" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The dependence of the three-particle charge-dependent correlator MEAN(COS(PHI(A)+COS(PHI(B)-2*PHI(RP)) on the PT difference between the two particles A and B for the centrality range 30-40%.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60510.v1/t9
title: "Table 9" of "Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV"

description: The dependence of the three-particle charge-dependent correlator MEAN(COS(PHI(A)+COS(PHI(B)-2*PHI(RP)) on the average PT of the two particles A and B for the centrality range 30-40%.
description: CERN-LHC. Measurements of charge dependent azimuthal correlations of charged particles produced in Lead-Lead collisions at a centre of mass energy per nucleon pair of 2.76 TeV. The data sample of about 13 million minimum bias events covers the |eta| range &lt;0.8 with data presented as a function of the collision centrality, particle separation in pseudorapidity and transverse momentum. Data for two-particle and three-particle correlation functions are presented. See the text of the paper for more details of the analysis. 
The indices A and B refer to the charge of the particle and the MEAN values are an average over the particle pairs within the event as well as an average over all analysed events.
DOI: 10.17182/hepdata.60518.v1/t1
title: "Table 1" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The fiducial and acceptance-corrected cross sections for PT&lt;50 GeV/c and |rapidity|&lt;2.4.
description: CERN-LHC. Measurement of the cross sections for Upsilon(1s), Upsilon(2S) and Upsilon(3S) production in proton-proton collisions at a centre of mass energy of 7 TeV. The data sample, with an integrated luminosity of 35.8+-1.4 pb-1 covers the PT range 0-50 GeV/c and |rapidity| &lt; 2.4. The Upsilon resonances are identified through their decay to di-muons and the data are uncorrected for the branching ratio. Fiducial as well as acceptance-corrected cross sections are tabulated. The effects of the polarization on the acceptance corrected cross section are given for the following extreme scenarios: 
HX_ T - fully transverse in the helicity frame 
HX_ L - fully longitudinal in the helicity frame 
CS_ T - fully transverse in the Collins-Soper frame 
CS_ L - fully longitudinal in the Collins-Soper frame.
DOI: 10.17182/hepdata.60518.v1/t2
title: "Table 2" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The fiducial and acceptance corrected UPSI(1S) production cross sections (times di-muon branching ratio) as a function of PT for the |rapidity| range &lt; 2.4. Note these are integrated cross sections and the acceptance-corrected cross sections assume the UPSI(1S) are unpolarized with the variations due to the 4 extreme polarization scenarios shown in the last 4 columns. The fiducial cross sections do not need to make any assumptions on the polarizations scenarios. The luminosity uncertainty of 4% is not included in the systematic errors.
description: CERN-LHC. Measurement of the cross sections for Upsilon(1s), Upsilon(2S) and Upsilon(3S) production in proton-proton collisions at a centre of mass energy of 7 TeV. The data sample, with an integrated luminosity of 35.8+-1.4 pb-1 covers the PT range 0-50 GeV/c and |rapidity| &lt; 2.4. The Upsilon resonances are identified through their decay to di-muons and the data are uncorrected for the branching ratio. Fiducial as well as acceptance-corrected cross sections are tabulated. The effects of the polarization on the acceptance corrected cross section are given for the following extreme scenarios: 
HX_ T - fully transverse in the helicity frame 
HX_ L - fully longitudinal in the helicity frame 
CS_ T - fully transverse in the Collins-Soper frame 
CS_ L - fully longitudinal in the Collins-Soper frame.
DOI: 10.17182/hepdata.60518.v1/t3
title: "Table 3" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The fiducial and acceptance corrected UPSI(2S) production cross sections (times di-muon branching ratio) as a function of PT for the |rapidity| range &lt; 2.4. Note these are integrated cross sections and the acceptance-corrected cross sections assume the UPSI(2S) are unpolarized with the variations due to the 4 extreme polarization scenarios shown in the last 4 columns. The fiducial cross sections do not need to make any assumptions on the polarizations scenarios. The luminosity uncertainty of 4% is not included in the systematic errors.
description: CERN-LHC. Measurement of the cross sections for Upsilon(1s), Upsilon(2S) and Upsilon(3S) production in proton-proton collisions at a centre of mass energy of 7 TeV. The data sample, with an integrated luminosity of 35.8+-1.4 pb-1 covers the PT range 0-50 GeV/c and |rapidity| &lt; 2.4. The Upsilon resonances are identified through their decay to di-muons and the data are uncorrected for the branching ratio. Fiducial as well as acceptance-corrected cross sections are tabulated. The effects of the polarization on the acceptance corrected cross section are given for the following extreme scenarios: 
HX_ T - fully transverse in the helicity frame 
HX_ L - fully longitudinal in the helicity frame 
CS_ T - fully transverse in the Collins-Soper frame 
CS_ L - fully longitudinal in the Collins-Soper frame.
DOI: 10.17182/hepdata.60518.v1/t4
title: "Table 4" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The fiducial and acceptance corrected UPSI(3S) production cross sections (times di-muon branching ratio) as a function of PT for the |rapidity| range &lt; 2.4. Note these are integrated cross sections and the acceptance-corrected cross sections assume the UPSI(3S) are unpolarized with the variations due to the 4 extreme polarization scenarios shown in the last 4 columns. The fiducial cross sections do not need to make any assumptions on the polarizations scenarios. The luminosity uncertainty of 4% is not included in the systematic errors.
description: CERN-LHC. Measurement of the cross sections for Upsilon(1s), Upsilon(2S) and Upsilon(3S) production in proton-proton collisions at a centre of mass energy of 7 TeV. The data sample, with an integrated luminosity of 35.8+-1.4 pb-1 covers the PT range 0-50 GeV/c and |rapidity| &lt; 2.4. The Upsilon resonances are identified through their decay to di-muons and the data are uncorrected for the branching ratio. Fiducial as well as acceptance-corrected cross sections are tabulated. The effects of the polarization on the acceptance corrected cross section are given for the following extreme scenarios: 
HX_ T - fully transverse in the helicity frame 
HX_ L - fully longitudinal in the helicity frame 
CS_ T - fully transverse in the Collins-Soper frame 
CS_ L - fully longitudinal in the Collins-Soper frame.
DOI: 10.17182/hepdata.60518.v1/t5
title: "Table 5" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The fiducial and acceptance corrected UPSI(1S) production cross sections (times di-muon branching ratio) as a function of PT for the |rapidity| range &lt; 0.4. Note these are integrated cross sections and the acceptance-corrected cross sections assume the UPSI(1S) are unpolarized with the variations due to the 4 extreme polarization scenarios shown in the last 4 columns. The fiducial cross sections do not need to make any assumptions on the polarizations scenarios. The luminosity uncertainty of 4% is not included in the systematic errors.
description: CERN-LHC. Measurement of the cross sections for Upsilon(1s), Upsilon(2S) and Upsilon(3S) production in proton-proton collisions at a centre of mass energy of 7 TeV. The data sample, with an integrated luminosity of 35.8+-1.4 pb-1 covers the PT range 0-50 GeV/c and |rapidity| &lt; 2.4. The Upsilon resonances are identified through their decay to di-muons and the data are uncorrected for the branching ratio. Fiducial as well as acceptance-corrected cross sections are tabulated. The effects of the polarization on the acceptance corrected cross section are given for the following extreme scenarios: 
HX_ T - fully transverse in the helicity frame 
HX_ L - fully longitudinal in the helicity frame 
CS_ T - fully transverse in the Collins-Soper frame 
CS_ L - fully longitudinal in the Collins-Soper frame.
DOI: 10.17182/hepdata.60518.v1/t6
title: "Table 6" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The fiducial and acceptance corrected UPSI(2S) production cross sections (times di-muon branching ratio) as a function of PT for the |rapidity| range &lt; 0.4. Note these are integrated cross sections and the acceptance-corrected cross sections assume the UPSI(2S) are unpolarized with the variations due to the 4 extreme polarization scenarios shown in the last 4 columns. The fiducial cross sections do not need to make any assumptions on the polarizations scenarios. The luminosity uncertainty of 4% is not included in the systematic errors.
description: CERN-LHC. Measurement of the cross sections for Upsilon(1s), Upsilon(2S) and Upsilon(3S) production in proton-proton collisions at a centre of mass energy of 7 TeV. The data sample, with an integrated luminosity of 35.8+-1.4 pb-1 covers the PT range 0-50 GeV/c and |rapidity| &lt; 2.4. The Upsilon resonances are identified through their decay to di-muons and the data are uncorrected for the branching ratio. Fiducial as well as acceptance-corrected cross sections are tabulated. The effects of the polarization on the acceptance corrected cross section are given for the following extreme scenarios: 
HX_ T - fully transverse in the helicity frame 
HX_ L - fully longitudinal in the helicity frame 
CS_ T - fully transverse in the Collins-Soper frame 
CS_ L - fully longitudinal in the Collins-Soper frame.