cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.60518.v1/t22
title: "Table 22" 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 2.0 to 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/t23
title: "Table 23" 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 rapidity for PT &lt; 50 GeV/c. 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/t24
title: "Table 24" 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 rapidity for PT &lt; 50 GeV/c. 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/t25
title: "Table 25" 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 rapidity for PT &lt; 50 GeV/c. 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/t26
title: "Table 26" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The ratios of the UPSI(3S) to UPSI(1S) fiducial and acceptance cross sections as a function of PT for the |rapidiy| range &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/t27
title: "Table 27" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The ratios of the UPSI(2S) to UPSI(1S) fiducial and acceptance cross sections as a function of PT for the |rapidiy| range &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/t28
title: "Table 28" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The ratios of the UPSI(3S) to UPSI(2S) fiducial and acceptance cross sections as a function of PT for the |rapidiy| range &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/t29
title: "Table 29" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The acceptance-corrected UPSI(1S) production cross section, integrated and differential in PT, times the respective dimuon branching fraction, integrated over the rapidity range |y| &lt; 1.2. The first (sys) error is the quadratic sum of all systematic uncertainties excluding that associated with the polarization of the UPSI(1S) which is shown separately as the second (sys) value. The latter has been obtained by calculating the acceptance with the +68 and -68% CL as given by the measured UPSI(1S) polarization [see. PRL 110 (2013) 081802].
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/t30
title: "Table 30" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The acceptance-corrected UPSI(2S) production cross section, integrated and differential in PT, times the respective dimuon branching fraction, integrated over the rapidity range |y| &lt; 1.2. The first (sys) error is the quadratic sum of all systematic uncertainties excluding that associated with the polarization of the UPSI(2S) which is shown separately as the second (sys) value. The latter has been obtained by calculating the acceptance with the +68 and -68% CL as given by the measured UPSI(2S) polarization [see. PRL 110 (2013) 081802].
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/t31
title: "Table 31" of "Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ Cross Sections in $pp$ Collisions at $\sqrt{s}$ = 7 TeV"

description: The acceptance-corrected UPSI(3S) production cross section, integrated and differential in PT, times the respective dimuon branching fraction, integrated over the rapidity range |y| &lt; 1.2. The first (sys) error is the quadratic sum of all systematic uncertainties excluding that associated with the polarization of the UPSI(3S) which is shown separately as the second (sys) value. The latter has been obtained by calculating the acceptance with the +68 and -68% CL as given by the measured UPSI(3S) polarization [see. PRL 110 (2013) 081802].
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.60522.v1/t2
title: "Table 2" of "Transverse momentum cross section of $e^+e^-$ pairs in the $Z$-boson region from $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV"

description: The differential PT cross section as a function of PT.
description: Fermilab-Tevatron. Measurement of the differential transverse momentum cross section for E+E- pairs in their invariant mass region of 66-116 GeV from antiproton-proton collisions at a centre of mass energy of 1.96 TeV. The data sample used has an integrated luminosity of 2.1 fb-1 taken during Run II and covers the PT region 0 to 21 GeV.
DOI: 10.17182/hepdata.60522.v1/t1
title: "Table 1" of "Transverse momentum cross section of $e^+e^-$ pairs in the $Z$-boson region from $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV"

description: Total integrated cross section.
description: Fermilab-Tevatron. Measurement of the differential transverse momentum cross section for E+E- pairs in their invariant mass region of 66-116 GeV from antiproton-proton collisions at a centre of mass energy of 1.96 TeV. The data sample used has an integrated luminosity of 2.1 fb-1 taken during Run II and covers the PT region 0 to 21 GeV.
DOI: 10.17182/hepdata.60556.v1/t1
title: "Table 1" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$ TeV"

description: The measured differential distribution in the two-photon mass;.
description: Fermilab-Tevatron. Measurements of the differential distributions of isolated direct photon pair production in antiproton-proton collisions at a centre-of-mass energy of 1.96 TeV. The data sample, with integrated luminosity 8.5 fb-1, is used to determine the photon pair differential mass distribution (DSIG/DMT), the transverse momentum distribution (DSIG/DPT), the distribution in the azimuthal angle between the two photons (DSIG/D(PHI1-DPHI2) and the polar scattering angle angle distribution in the Collins-Soper frame (DSIG/D|COS(THETA*)|. The measurements require isolated photons with PT &gt; 18 (17) for the leading (next-to-leading) photons having |eta|&lt;0.9 and separation from each other in eta-phi space &gt; 0.4.
DOI: 10.17182/hepdata.60556.v1/t2
title: "Table 2" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$ TeV"

description: The measured differential distribution in the two-photon transverse momentum;.
description: Fermilab-Tevatron. Measurements of the differential distributions of isolated direct photon pair production in antiproton-proton collisions at a centre-of-mass energy of 1.96 TeV. The data sample, with integrated luminosity 8.5 fb-1, is used to determine the photon pair differential mass distribution (DSIG/DMT), the transverse momentum distribution (DSIG/DPT), the distribution in the azimuthal angle between the two photons (DSIG/D(PHI1-DPHI2) and the polar scattering angle angle distribution in the Collins-Soper frame (DSIG/D|COS(THETA*)|. The measurements require isolated photons with PT &gt; 18 (17) for the leading (next-to-leading) photons having |eta|&lt;0.9 and separation from each other in eta-phi space &gt; 0.4.
DOI: 10.17182/hepdata.60556.v1/t4
title: "Table 4" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$ TeV"

description: The measured differential distribution in the polar scattering angle in the Collins-Soper frame;.
description: Fermilab-Tevatron. Measurements of the differential distributions of isolated direct photon pair production in antiproton-proton collisions at a centre-of-mass energy of 1.96 TeV. The data sample, with integrated luminosity 8.5 fb-1, is used to determine the photon pair differential mass distribution (DSIG/DMT), the transverse momentum distribution (DSIG/DPT), the distribution in the azimuthal angle between the two photons (DSIG/D(PHI1-DPHI2) and the polar scattering angle angle distribution in the Collins-Soper frame (DSIG/D|COS(THETA*)|. The measurements require isolated photons with PT &gt; 18 (17) for the leading (next-to-leading) photons having |eta|&lt;0.9 and separation from each other in eta-phi space &gt; 0.4.
DOI: 10.17182/hepdata.60556.v1/t3
title: "Table 3" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$ TeV"

description: The measured differential distribution in the azimuthal angular separation of the two photons;.
description: Fermilab-Tevatron. Measurements of the differential distributions of isolated direct photon pair production in antiproton-proton collisions at a centre-of-mass energy of 1.96 TeV. The data sample, with integrated luminosity 8.5 fb-1, is used to determine the photon pair differential mass distribution (DSIG/DMT), the transverse momentum distribution (DSIG/DPT), the distribution in the azimuthal angle between the two photons (DSIG/D(PHI1-DPHI2) and the polar scattering angle angle distribution in the Collins-Soper frame (DSIG/D|COS(THETA*)|. The measurements require isolated photons with PT &gt; 18 (17) for the leading (next-to-leading) photons having |eta|&lt;0.9 and separation from each other in eta-phi space &gt; 0.4.
DOI: 10.17182/hepdata.60556.v1/t5
title: "Table 5" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$ TeV"

description: The measured differential distribution in the two-photon mass for |azimuthal angle separation| &lt; PI/2;.
description: Fermilab-Tevatron. Measurements of the differential distributions of isolated direct photon pair production in antiproton-proton collisions at a centre-of-mass energy of 1.96 TeV. The data sample, with integrated luminosity 8.5 fb-1, is used to determine the photon pair differential mass distribution (DSIG/DMT), the transverse momentum distribution (DSIG/DPT), the distribution in the azimuthal angle between the two photons (DSIG/D(PHI1-DPHI2) and the polar scattering angle angle distribution in the Collins-Soper frame (DSIG/D|COS(THETA*)|. The measurements require isolated photons with PT &gt; 18 (17) for the leading (next-to-leading) photons having |eta|&lt;0.9 and separation from each other in eta-phi space &gt; 0.4.
DOI: 10.17182/hepdata.60556.v1/t6
title: "Table 6" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$ TeV"

description: The measured differential distribution in the two-photon transverse momentum for |azimuthal angle separation| &lt; PI/2;.
description: Fermilab-Tevatron. Measurements of the differential distributions of isolated direct photon pair production in antiproton-proton collisions at a centre-of-mass energy of 1.96 TeV. The data sample, with integrated luminosity 8.5 fb-1, is used to determine the photon pair differential mass distribution (DSIG/DMT), the transverse momentum distribution (DSIG/DPT), the distribution in the azimuthal angle between the two photons (DSIG/D(PHI1-DPHI2) and the polar scattering angle angle distribution in the Collins-Soper frame (DSIG/D|COS(THETA*)|. The measurements require isolated photons with PT &gt; 18 (17) for the leading (next-to-leading) photons having |eta|&lt;0.9 and separation from each other in eta-phi space &gt; 0.4.
DOI: 10.17182/hepdata.60556.v1/t7
title: "Table 7" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$ TeV"

description: The measured differential distribution in the polar scattering angle in the Collins-Soper frame for |azimuthal angle separation| &lt; PI/2;.
description: Fermilab-Tevatron. Measurements of the differential distributions of isolated direct photon pair production in antiproton-proton collisions at a centre-of-mass energy of 1.96 TeV. The data sample, with integrated luminosity 8.5 fb-1, is used to determine the photon pair differential mass distribution (DSIG/DMT), the transverse momentum distribution (DSIG/DPT), the distribution in the azimuthal angle between the two photons (DSIG/D(PHI1-DPHI2) and the polar scattering angle angle distribution in the Collins-Soper frame (DSIG/D|COS(THETA*)|. The measurements require isolated photons with PT &gt; 18 (17) for the leading (next-to-leading) photons having |eta|&lt;0.9 and separation from each other in eta-phi space &gt; 0.4.
DOI: 10.17182/hepdata.60556.v1/t8
title: "Table 8" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$ TeV"

description: The measured differential distribution in the two-photon mass for |azimuthal angle separation| &gt; PI/2;.
description: Fermilab-Tevatron. Measurements of the differential distributions of isolated direct photon pair production in antiproton-proton collisions at a centre-of-mass energy of 1.96 TeV. The data sample, with integrated luminosity 8.5 fb-1, is used to determine the photon pair differential mass distribution (DSIG/DMT), the transverse momentum distribution (DSIG/DPT), the distribution in the azimuthal angle between the two photons (DSIG/D(PHI1-DPHI2) and the polar scattering angle angle distribution in the Collins-Soper frame (DSIG/D|COS(THETA*)|. The measurements require isolated photons with PT &gt; 18 (17) for the leading (next-to-leading) photons having |eta|&lt;0.9 and separation from each other in eta-phi space &gt; 0.4.