cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.73234.v1/t4
title: "Table 4" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential cross sections as a function of the variable $z_{I\!\!P}$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t10
title: "Table 10" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t11
title: "Table 11" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $\langle\eta^{\text{jets}}\rangle$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t13
title: "Table 13" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $x_{I\!\!P}$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t5
title: "Table 5" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential cross sections as a function of the variable $x_{I\!\!P}$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t6
title: "Table 6" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential cross sections as a function of the variable $y$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t7
title: "Table 7" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential cross sections as a function of the variable $Q^2$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t8
title: "Table 8" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t9
title: "Table 9" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $M_X$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t12
title: "Table 12" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $z_{I\!\!P}$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t14
title: "Table 14" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $y$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t15
title: "Table 15" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $x_\gamma$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t16
title: "Table 16" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t17
title: "Table 17" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $M_X$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t18
title: "Table 18" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t19
title: "Table 19" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $\langle\eta^{\text{jets}}\rangle$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t20
title: "Table 20" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t21
title: "Table 21" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $y$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t22
title: "Table 22" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $z_{I\!\!P}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73234.v1/t23
title: "Table 23" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.
description: DESY-HERA. The cross section of the diffractive process e^+p -&gt; e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 &lt;2 GeV^2 and in deep-inelastic scattering with 4 GeV^2
DOI: 10.17182/hepdata.73235.v1/t1
title: "Table 1" of "Effect of event selection on jetlike correlation measurement in $d$+Au collisions at $\sqrt{s_{\rm{NN}}}=200$ GeV"

description: The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the near (|$\Delta\phi$| &lt; $\pi$/3). Shown is the low FTPC-Au activity data. Trigger and associated particles have 1 &lt; $p_T$ &lt; 3 GeV/c and |$\eta$| &lt; 1.
description: BNL-RHIC. Dihadron correlations are analyzed in $\sqrt{s_{_{\rm NN}}} = 200$ GeV $d$+Au collisions classified by forward charged particle multiplicity and zero-degree neutral energy in the Au-beam direction. It is found that the jetlike correlated yield increases with the event multiplicity. After taking into account this dependence, the non-jet contribution on the away side is minimal, leaving little room for a back-to-back ridge in these collisions.
DOI: 10.17182/hepdata.73235.v1/t2
title: "Table 2" of "Effect of event selection on jetlike correlation measurement in $d$+Au collisions at $\sqrt{s_{\rm{NN}}}=200$ GeV"

description: The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| &lt; $\pi$/3. Shown is the high FTPC-Au activity data. Trigger and associated particles have 1 &lt; $p_T$ &lt; 3 GeV/c and |$\eta$| &lt; 1.
description: BNL-RHIC. Dihadron correlations are analyzed in $\sqrt{s_{_{\rm NN}}} = 200$ GeV $d$+Au collisions classified by forward charged particle multiplicity and zero-degree neutral energy in the Au-beam direction. It is found that the jetlike correlated yield increases with the event multiplicity. After taking into account this dependence, the non-jet contribution on the away side is minimal, leaving little room for a back-to-back ridge in these collisions.
DOI: 10.17182/hepdata.73235.v1/t3
title: "Table 3" of "Effect of event selection on jetlike correlation measurement in $d$+Au collisions at $\sqrt{s_{\rm{NN}}}=200$ GeV"

description: The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the near (|$\Delta\phi$| &lt; $\pi$/3) side. Shown is the high-activity data after subtracting the unscaled. Trigger and associated particles have 1 &lt; $p_T$ &lt; 3 GeV/c and |$\eta$| &lt; 1.
description: BNL-RHIC. Dihadron correlations are analyzed in $\sqrt{s_{_{\rm NN}}} = 200$ GeV $d$+Au collisions classified by forward charged particle multiplicity and zero-degree neutral energy in the Au-beam direction. It is found that the jetlike correlated yield increases with the event multiplicity. After taking into account this dependence, the non-jet contribution on the away side is minimal, leaving little room for a back-to-back ridge in these collisions.
DOI: 10.17182/hepdata.73235.v1/t4
title: "Table 4" of "Effect of event selection on jetlike correlation measurement in $d$+Au collisions at $\sqrt{s_{\rm{NN}}}=200$ GeV"

description: The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| &lt; $\pi$/3). Shown is the high FTPC-Au activity data. Trigger and associated particles have 1 &lt; $p_T$ &lt; 3 GeV/c and |$\eta$| &lt; 1.
description: BNL-RHIC. Dihadron correlations are analyzed in $\sqrt{s_{_{\rm NN}}} = 200$ GeV $d$+Au collisions classified by forward charged particle multiplicity and zero-degree neutral energy in the Au-beam direction. It is found that the jetlike correlated yield increases with the event multiplicity. After taking into account this dependence, the non-jet contribution on the away side is minimal, leaving little room for a back-to-back ridge in these collisions.
DOI: 10.17182/hepdata.73235.v1/t5
title: "Table 5" of "Effect of event selection on jetlike correlation measurement in $d$+Au collisions at $\sqrt{s_{\rm{NN}}}=200$ GeV"

description: The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| &lt; $\pi$/3). Shown is the high-activity data after subtracting the unscaled low-activity data. Trigger and associated particles have 1 &lt; $p_T$ &lt; 3 GeV/c and |$\eta$| &lt; 1.
description: BNL-RHIC. Dihadron correlations are analyzed in $\sqrt{s_{_{\rm NN}}} = 200$ GeV $d$+Au collisions classified by forward charged particle multiplicity and zero-degree neutral energy in the Au-beam direction. It is found that the jetlike correlated yield increases with the event multiplicity. After taking into account this dependence, the non-jet contribution on the away side is minimal, leaving little room for a back-to-back ridge in these collisions.
DOI: 10.17182/hepdata.73235.v1/t6
title: "Table 6" of "Effect of event selection on jetlike correlation measurement in $d$+Au collisions at $\sqrt{s_{\rm{NN}}}=200$ GeV"

description: The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| &lt; $\pi$/3). Shown is the high-activity data after subtracting the unscaled low-activity data. Trigger and associated particles have 1 &lt; $p_T$ &lt; 3 GeV/c and |$\eta$| &lt; 1.
description: BNL-RHIC. Dihadron correlations are analyzed in $\sqrt{s_{_{\rm NN}}} = 200$ GeV $d$+Au collisions classified by forward charged particle multiplicity and zero-degree neutral energy in the Au-beam direction. It is found that the jetlike correlated yield increases with the event multiplicity. After taking into account this dependence, the non-jet contribution on the away side is minimal, leaving little room for a back-to-back ridge in these collisions.