cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.73177.v1/t1
title: "Table 1" of "Measurement of the electron charge asymmetry in $\boldsymbol{p\bar{p}\rightarrow W+X \rightarrow e\nu +X}$ decays in $\boldsymbol{p\bar{p}}$ collisions at $\boldsymbol{\sqrt{s}=1.96}$ TeV"

description: CP-folded electron charge asymmetry for data with $E_T^{e} &gt; 25$ GeV multiplied by 100.
$\langle|\eta^e|\rangle$ is the cross section weighted average of electron pseudorapidity in each bin from RESBOS with PHOTOS.
description: FNAL-Tevatron. We present a measurement of the electron charge asymmetry in $p\bar{p}\rightarrow W+X \rightarrow e\nu +X$ events at a center-of-mass energy of 1.96 TeV, using data corresponding to 9.7 fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider. The asymmetry is measured as a function of the electron pseudorapidity and is presented in five kinematic bins based on the electron transverse energy and the missing transverse energy in the event. The measured asymmetry is compared with next-to-leading-order predictions in perturbative quantum chromodynamics and provides accurate information for the determination of parton distribution functions of the proton. This is the most precise lepton charge asymmetry measurement to date.
DOI: 10.17182/hepdata.73177.v1/t2
title: "Table 2" of "Measurement of the electron charge asymmetry in $\boldsymbol{p\bar{p}\rightarrow W+X \rightarrow e\nu +X}$ decays in $\boldsymbol{p\bar{p}}$ collisions at $\boldsymbol{\sqrt{s}=1.96}$ TeV"

description: CP-folded electron charge asymmetry for data with $25 &lt; E_T^{e} &lt; 35$ GeV multiplied by 100.
$\langle|\eta^e|\rangle$ is the cross section weighted average of electron pseudorapidity in each bin from RESBOS with PHOTOS.
description: FNAL-Tevatron. We present a measurement of the electron charge asymmetry in $p\bar{p}\rightarrow W+X \rightarrow e\nu +X$ events at a center-of-mass energy of 1.96 TeV, using data corresponding to 9.7 fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider. The asymmetry is measured as a function of the electron pseudorapidity and is presented in five kinematic bins based on the electron transverse energy and the missing transverse energy in the event. The measured asymmetry is compared with next-to-leading-order predictions in perturbative quantum chromodynamics and provides accurate information for the determination of parton distribution functions of the proton. This is the most precise lepton charge asymmetry measurement to date.
DOI: 10.17182/hepdata.73177.v1/t3
title: "Table 3" of "Measurement of the electron charge asymmetry in $\boldsymbol{p\bar{p}\rightarrow W+X \rightarrow e\nu +X}$ decays in $\boldsymbol{p\bar{p}}$ collisions at $\boldsymbol{\sqrt{s}=1.96}$ TeV"

description: CP-folded electron charge asymmetry for data with $E_T^{e} &gt; 35$ GeV multiplied by 100.
$\langle|\eta^e|\rangle$ is the cross section weighted average of electron pseudorapidity in each bin from RESBOS with PHOTOS.
description: FNAL-Tevatron. We present a measurement of the electron charge asymmetry in $p\bar{p}\rightarrow W+X \rightarrow e\nu +X$ events at a center-of-mass energy of 1.96 TeV, using data corresponding to 9.7 fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider. The asymmetry is measured as a function of the electron pseudorapidity and is presented in five kinematic bins based on the electron transverse energy and the missing transverse energy in the event. The measured asymmetry is compared with next-to-leading-order predictions in perturbative quantum chromodynamics and provides accurate information for the determination of parton distribution functions of the proton. This is the most precise lepton charge asymmetry measurement to date.
DOI: 10.17182/hepdata.73182.v1/t1
title: "Table 1" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

description: Total $\nu_\mu$ CC1$\pi^+$ cross section on water in the reduced phase-space of $p_{\pi^+} &gt; 200$ MeV/$c$, $p_\mu &gt; 200$ MeV/c, $\cos(\theta_{\pi^+}) &gt; 0.3$ and $\cos(\theta_\mu) &gt; 0.3$. The T2K data point is placed at the $\nu_\mu$ flux mean energy.
description: KEK. The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$ GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+} &gt; 200$ MeV/c, $p_{\mu^-} &gt; 200$ MeV/c, $\cos\theta_{\pi^+} &gt; 0.3$ and $\cos\theta_{\mu^-} &gt; 0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$.

Data points taken from attached tar file available at http://t2k-experiment.org/results/.
DOI: 10.17182/hepdata.73182.v1/t2
title: "Table 2" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

description: Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $p_\pi$ in the reduced phase-space of $p_{\pi^+} &gt; 200$ MeV/$c$, $p_\mu &gt; 200$ MeV/c, $\cos(\theta_{\pi^+}) &gt; 0.3$ and $\cos(\theta_\mu) &gt; 0.3$.
description: KEK. The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$ GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+} &gt; 200$ MeV/c, $p_{\mu^-} &gt; 200$ MeV/c, $\cos\theta_{\pi^+} &gt; 0.3$ and $\cos\theta_{\mu^-} &gt; 0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$.

Data points taken from attached tar file available at http://t2k-experiment.org/results/.
DOI: 10.15468/dl.ubq7qv
title: Occurrence Download

description: A dataset containing 16 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (Sorbus glabriuscula)",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "Year is greater than or equal to 1981",
 "OccurrenceStatus is Present",
 {
 "not" : {
 "BasisOfRecord" : [
 "is one of (Fossil, Living Specimen)"
 ]
 }
 },
 "Geometry POLYGON((-180 -90,180 -90,180 90,-180 90,-180 -90))"
 ]
}

 The dataset includes 16 records from 8 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015354-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.73182.v1/t3
title: "Table 3" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

description: Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $\cos\theta_\pi$ in the reduced phase-space of $p_{\pi^+} &gt; 200$ MeV/$c$, $p_\mu &gt; 200$ MeV/c, $\cos(\theta_{\pi^+}) &gt; 0.3$ and $\cos(\theta_\mu) &gt; 0.3$.
description: KEK. The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$ GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+} &gt; 200$ MeV/c, $p_{\mu^-} &gt; 200$ MeV/c, $\cos\theta_{\pi^+} &gt; 0.3$ and $\cos\theta_{\mu^-} &gt; 0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$.

Data points taken from attached tar file available at http://t2k-experiment.org/results/.
DOI: 10.17182/hepdata.73182.v1/t4
title: "Table 4" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

description: Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $p_\mu$ in the reduced phase-space of $p_{\pi^+} &gt; 200$ MeV/$c$, $p_\mu &gt; 200$ MeV/c, $\cos(\theta_{\pi^+}) &gt; 0.3$ and $\cos(\theta_\mu) &gt; 0.3$.
description: KEK. The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$ GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+} &gt; 200$ MeV/c, $p_{\mu^-} &gt; 200$ MeV/c, $\cos\theta_{\pi^+} &gt; 0.3$ and $\cos\theta_{\mu^-} &gt; 0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$.

Data points taken from attached tar file available at http://t2k-experiment.org/results/.
DOI: 10.17182/hepdata.73182.v1/t5
title: "Table 5" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

description: Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $\cos\theta_\mu$ in the reduced phase-space of $p_{\pi^+} &gt; 200$ MeV/$c$, $p_\mu &gt; 200$ MeV/c, $\cos(\theta_{\pi^+}) &gt; 0.3$ and $\cos(\theta_\mu) &gt; 0.3$.
description: KEK. The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$ GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+} &gt; 200$ MeV/c, $p_{\mu^-} &gt; 200$ MeV/c, $\cos\theta_{\pi^+} &gt; 0.3$ and $\cos\theta_{\mu^-} &gt; 0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$.

Data points taken from attached tar file available at http://t2k-experiment.org/results/.
DOI: 10.17182/hepdata.73182.v1/t6
title: "Table 6" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

description: Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $\cos\theta_{\mu,\pi}$ in the reduced phase-space of $p_{\pi^+} &gt; 200$ MeV/$c$, $p_\mu &gt; 200$ MeV/c, $\cos(\theta_{\pi^+}) &gt; 0.3$ and $\cos(\theta_\mu) &gt; 0.3$.
description: KEK. The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$ GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+} &gt; 200$ MeV/c, $p_{\mu^-} &gt; 200$ MeV/c, $\cos\theta_{\pi^+} &gt; 0.3$ and $\cos\theta_{\mu^-} &gt; 0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$.

Data points taken from attached tar file available at http://t2k-experiment.org/results/.
DOI: 10.17182/hepdata.73182.v1/t7
title: "Table 7" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

description: Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $E_\nu^{\rm rec}$ ($\Delta$) in the reduced phase-space of $p_{\pi^+} &gt; 200$ MeV/$c$, $p_\mu &gt; 200$ MeV/c, $\cos(\theta_{\pi^+}) &gt; 0.3$ and $\cos(\theta_\mu) &gt; 0.3$.
description: KEK. The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$ GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+} &gt; 200$ MeV/c, $p_{\mu^-} &gt; 200$ MeV/c, $\cos\theta_{\pi^+} &gt; 0.3$ and $\cos\theta_{\mu^-} &gt; 0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$.

Data points taken from attached tar file available at http://t2k-experiment.org/results/.
DOI: 10.17182/hepdata.73182.v1/t8
title: "Table 8" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

description: Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $E_\nu^{\rm rec}$ ($\mu$, $\pi$) in the reduced phase-space of $p_{\pi^+} &gt; 200$ MeV/$c$, $p_\mu &gt; 200$ MeV/c, $\cos(\theta_{\pi^+}) &gt; 0.3$ and $\cos(\theta_\mu) &gt; 0.3$.
description: KEK. The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$ GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+} &gt; 200$ MeV/c, $p_{\mu^-} &gt; 200$ MeV/c, $\cos\theta_{\pi^+} &gt; 0.3$ and $\cos\theta_{\mu^-} &gt; 0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$.

Data points taken from attached tar file available at http://t2k-experiment.org/results/.
DOI: 10.6084/m9.figshare.29950388.v1
title: Adaptive radiation during long-term experimental evolution of the multicellular bacterium, <i>Streptomyces</i>

description: The rapid diversification of a single lineage into novel ecological niches underpins evolution of biodiversity, with adaptive radiations being important drivers of ecological diversity across the tree of life. Experimental evolution has revolutionised our understanding of the fundamental ecological and evolutionary processes in adaptation. To study adaptation in the industrially and ecologically important bacterium <i>Streptomyces, </i>a long-term evolution experiment (LTEE) was undertaken in a strain lacking several antibiotic biosynthetic gene clusters (BGCs), facilitating the study of epistasis in antibiotic biosynthesis. <i>Streptomyces coelicolor </i>is a filamentous soil organism that does not undergo sporulation under the LTEE conditions, affording the opportunity to study adaptation under relaxed selection on sporulation. Replicate populations showed parallel loss of sporulation and major morphological shifts in terms of hyphal growth and aggregate formation, where fragmenting hyphae became the dominant phenotype. Catabolic diversification was also evident across the replicate populations with extensive growth rate changes relative to the progenitor across several nutrient sources, where there is evidence for both antagonistic pleiotropy and mutation accumulation. Negative epistasis was predominant in antibiotic biosynthesis in strains from the LTEE. This system provides a foundation for studying diversification and adaption to a novel environment in a physiologically and morphologically complex organism.Code associated with the Streptomyces LTEE is here https://github.com/PaulHoskisson/StreptomycesLTEE/tree/main<br><br>
DOI: 10.17182/hepdata.71987.v1/t59
title: "Table 59" of "Search for new phenomena in final states with large jet multiplicities and missing transverse momentum with ATLAS using $\sqrt{s} =13$ TeV proton--proton collisions"

description: Performance of the 9j50-0b selection for the 2Step grid: number of generated signal events; total signal cross-section; acceptance; efficiency (fractional); observed CL using this region alone; expected CL using this region alone.
description: CERN-LHC. Results are reported of a search for new phenomena, such as supersymmetric particle production, that could be observed in high-energy proton--proton collisions. Events with large numbers of jets, together with missing transverse momentum from unobserved particles, are selected. The data analysed were recorded by the ATLAS experiment during 2015 using the 13 TeV centre-of-mass proton--proton collisions at the Large Hadron Collider, and correspond to an integrated luminosity of 3.2 fb$^{-1}$. The search selected events with various jet multiplicities from $\ge 7$ to $\ge 10$ jets, and with various $b$-jet multiplicity requirements to enhance sensitivity. No excess above Standard Model expectations is observed. The results are interpreted within two supersymmetry models, where gluino masses up to 1400 GeV are excluded at 95% confidence level, significantly extending previous limits.
DOI: 10.17182/hepdata.71987.v1/t60
title: "Table 60" of "Search for new phenomena in final states with large jet multiplicities and missing transverse momentum with ATLAS using $\sqrt{s} =13$ TeV proton--proton collisions"

description: Performance of the 9j50-1b selection for the 2Step grid: number of generated signal events; total signal cross-section; acceptance; efficiency (fractional); observed CL using this region alone; expected CL using this region alone.
description: CERN-LHC. Results are reported of a search for new phenomena, such as supersymmetric particle production, that could be observed in high-energy proton--proton collisions. Events with large numbers of jets, together with missing transverse momentum from unobserved particles, are selected. The data analysed were recorded by the ATLAS experiment during 2015 using the 13 TeV centre-of-mass proton--proton collisions at the Large Hadron Collider, and correspond to an integrated luminosity of 3.2 fb$^{-1}$. The search selected events with various jet multiplicities from $\ge 7$ to $\ge 10$ jets, and with various $b$-jet multiplicity requirements to enhance sensitivity. No excess above Standard Model expectations is observed. The results are interpreted within two supersymmetry models, where gluino masses up to 1400 GeV are excluded at 95% confidence level, significantly extending previous limits.
DOI: 10.17182/hepdata.73191.v1/t1
title: "Table 1" of "Measurement of the $W+b$-jet and $W+c$-jet differential production cross sections in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV"

description: The $W + b$-jet production cross sections times $W \to \mu\nu$ branching fraction, ${\rm d}\sigma/{\rm d}p_T^{\rm jet}$.
description: Fermilab-Tevatron. We present a measurement of the cross sections for the associated production of a $W$ boson with at least one heavy quark jet, $b$ or $c$, in proton-antiproton collisions. Data corresponding to an integrated luminosity of 8.7 fb$^{-1}$ recorded with the D0 detector at the Fermilab Tevatron $p\bar{p}$ Collider at $\sqrt{s}=1.96$ TeV are used to measure the cross sections differentially as a function of the jet transverse momenta in the range 20 to 150 GeV.
DOI: 10.17182/hepdata.73191.v1/t2
title: "Table 2" of "Measurement of the $W+b$-jet and $W+c$-jet differential production cross sections in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV"

description: The $W + c$-jet production cross sections times $W \to \mu\nu$ branching fraction, ${\rm d}\sigma/{\rm d}p_T^{\rm jet}$.
description: Fermilab-Tevatron. We present a measurement of the cross sections for the associated production of a $W$ boson with at least one heavy quark jet, $b$ or $c$, in proton-antiproton collisions. Data corresponding to an integrated luminosity of 8.7 fb$^{-1}$ recorded with the D0 detector at the Fermilab Tevatron $p\bar{p}$ Collider at $\sqrt{s}=1.96$ TeV are used to measure the cross sections differentially as a function of the jet transverse momenta in the range 20 to 150 GeV.
DOI: 10.17182/hepdata.73191.v1/t3
title: "Table 3" of "Measurement of the $W+b$-jet and $W+c$-jet differential production cross sections in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV"

description: The $\sigma(W+c)/\sigma(W+b)$ cross section ratio in bins of $c(b)$-jet $p_T$.
description: Fermilab-Tevatron. We present a measurement of the cross sections for the associated production of a $W$ boson with at least one heavy quark jet, $b$ or $c$, in proton-antiproton collisions. Data corresponding to an integrated luminosity of 8.7 fb$^{-1}$ recorded with the D0 detector at the Fermilab Tevatron $p\bar{p}$ Collider at $\sqrt{s}=1.96$ TeV are used to measure the cross sections differentially as a function of the jet transverse momenta in the range 20 to 150 GeV.
DOI: 10.17182/hepdata.73234.v1/t1
title: "Table 1" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Integrated $e^{+}p$ diffractive dijet cross sections in $\gamma p$. The hadronisation correction factor ($1+\delta_{\text{hadr}}$) applied to the NLO calculation is 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/t2
title: "Table 2" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Integrated $e^{+}p$ diffractive dijet cross sections in DIS. The hadronisation correction factor ($1+\delta_{\text{hadr}}$) applied to the NLO calculation and the radiative correction ($1+\delta_{\text{rad}}$) 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/t3
title: "Table 3" of "Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA"

description: Ratio of integrated $e^{+}p$ diffractive dijet cross sections for $Q^2&lt;2\,\text{GeV}^2$ (photoproduction) to $Q^2&gt;4\,\text{GeV}^2$ (DIS).
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