cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.66462.v1/t44
title: "Table 44" of "Searches for heavy long-lived charged particles with the ATLAS detector in proton-proton collisions at $\\sqrt{s}$ = 8 TeV"

description: Full-detector search R-Hadron candidate requirements and example candidate selection flow for combined selection.
description: CERN-LHC. Searches for heavy long-lived charged particles are performed using a data sample of 19.8 fb$^{-1}$ from proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 8 TeV collected by the ATLAS detector at the Large Hadron Collider. No excess is observed above the estimated background and limits are placed on the mass of long-lived particles in various supersymmetric models. Long-lived tau sleptons in models with gauge-mediated symmetry breaking are excluded up to masses between 440 and 385 GeV for $\tan\beta$ between 10 and 50, with a 290 GeV limit in the case where only direct tau slepton production is considered. In the context of simplified LeptoSUSY models, where sleptons are stable and have a mass of 300 GeV, squark and gluino masses are excluded up to a mass of 1500 and 1360 GeV, respectively. Directly produced charginos, in simplified models where they are nearly degenerate to the lightest neutralino, are excluded up to a mass of 620 GeV. $R$-hadrons, composites containing a gluino, bottom squark or top squark, are excluded up to a mass of 1270, 845 and 900 GeV, respectively, using the full detector; and up to a mass of 1260, 835 and 870 GeV using an approach disregarding information from the muon spectrometer.
DOI: 10.17182/hepdata.66507.v1/t1
title: "Table 1" of "Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA"

description: The elastic photoproduction cross section derived from the high-energy data set as a function of the photon-proton centre-of-mass energy W. PHI_T is the transeverse polarised photon flux.
description: DESY-HERA. Cross sections for elastic and proton-dissociative photoproduction of J/psi mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at -of-mass energies sqrt{s} approx 318 GeV and sqrt{s} approx 225 GeV, corresponding to integrated luminosities of L = 130 pb^{-1} and L = 10.8 pb^{-1}, respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25&lt; Wgp &lt; 110 GeV. Differential cross sections mathrm{d}sigma / mathrm{d}t where the squared four-momentum transfer at the proton vertex, are measured in the range 0t| &lt; 1.2 , gevsq the elastic process and 0t| &lt; 8 , gevsq proton dissociation. The results are compared to other measurements. The Wgp 0dependences are parametrised using phenomenological fits.
DOI: 10.17182/hepdata.66507.v1/t2
title: "Table 2" of "Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA"

description: The proton-dissociative photoproduction cross section derived from the high-energy data set as a function of the photon-proton centre-of-mass energy W. PHI_T is the transeverse polarised photon flux.
description: DESY-HERA. Cross sections for elastic and proton-dissociative photoproduction of J/psi mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at -of-mass energies sqrt{s} approx 318 GeV and sqrt{s} approx 225 GeV, corresponding to integrated luminosities of L = 130 pb^{-1} and L = 10.8 pb^{-1}, respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25&lt; Wgp &lt; 110 GeV. Differential cross sections mathrm{d}sigma / mathrm{d}t where the squared four-momentum transfer at the proton vertex, are measured in the range 0t| &lt; 1.2 , gevsq the elastic process and 0t| &lt; 8 , gevsq proton dissociation. The results are compared to other measurements. The Wgp 0dependences are parametrised using phenomenological fits.
DOI: 10.17182/hepdata.66507.v1/t3
title: "Table 3" of "Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA"

description: The elastic photoproduction cross section derived from the low-energy data set as a function of the photon-proton centre-of-mass energy W. PHI_T is the transeverse polarised photon flux.
description: DESY-HERA. Cross sections for elastic and proton-dissociative photoproduction of J/psi mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at -of-mass energies sqrt{s} approx 318 GeV and sqrt{s} approx 225 GeV, corresponding to integrated luminosities of L = 130 pb^{-1} and L = 10.8 pb^{-1}, respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25&lt; Wgp &lt; 110 GeV. Differential cross sections mathrm{d}sigma / mathrm{d}t where the squared four-momentum transfer at the proton vertex, are measured in the range 0t| &lt; 1.2 , gevsq the elastic process and 0t| &lt; 8 , gevsq proton dissociation. The results are compared to other measurements. The Wgp 0dependences are parametrised using phenomenological fits.
DOI: 10.17182/hepdata.66507.v1/t4
title: "Table 4" of "Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA"

description: The proton-dissociative photoproduction cross section derived from the low-energy data set as a function of the photon-proton centre-of-mass energy W. PHI_T is the transeverse polarised photon flux.
description: DESY-HERA. Cross sections for elastic and proton-dissociative photoproduction of J/psi mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at -of-mass energies sqrt{s} approx 318 GeV and sqrt{s} approx 225 GeV, corresponding to integrated luminosities of L = 130 pb^{-1} and L = 10.8 pb^{-1}, respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25&lt; Wgp &lt; 110 GeV. Differential cross sections mathrm{d}sigma / mathrm{d}t where the squared four-momentum transfer at the proton vertex, are measured in the range 0t| &lt; 1.2 , gevsq the elastic process and 0t| &lt; 8 , gevsq proton dissociation. The results are compared to other measurements. The Wgp 0dependences are parametrised using phenomenological fits.
DOI: 10.17182/hepdata.66507.v1/t5
title: "Table 5" of "Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA"

description: The elastic photoproduction differential cross section derived from the high-energy data set as a function of the negative squared momentum transfer at the proton vertex T.
UPDATE (27 JAN 2017): corrected 0.31 to 0.41 as centre of sixth bin.
description: DESY-HERA. Cross sections for elastic and proton-dissociative photoproduction of J/psi mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at -of-mass energies sqrt{s} approx 318 GeV and sqrt{s} approx 225 GeV, corresponding to integrated luminosities of L = 130 pb^{-1} and L = 10.8 pb^{-1}, respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25&lt; Wgp &lt; 110 GeV. Differential cross sections mathrm{d}sigma / mathrm{d}t where the squared four-momentum transfer at the proton vertex, are measured in the range 0t| &lt; 1.2 , gevsq the elastic process and 0t| &lt; 8 , gevsq proton dissociation. The results are compared to other measurements. The Wgp 0dependences are parametrised using phenomenological fits.
DOI: 10.17182/hepdata.66507.v1/t6
title: "Table 6" of "Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA"

description: The proton-dissociative photoproduction differential cross section derived from the high-energy data set as a function of the negative squared momentum transfer at the proton vertex T.
description: DESY-HERA. Cross sections for elastic and proton-dissociative photoproduction of J/psi mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at -of-mass energies sqrt{s} approx 318 GeV and sqrt{s} approx 225 GeV, corresponding to integrated luminosities of L = 130 pb^{-1} and L = 10.8 pb^{-1}, respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25&lt; Wgp &lt; 110 GeV. Differential cross sections mathrm{d}sigma / mathrm{d}t where the squared four-momentum transfer at the proton vertex, are measured in the range 0t| &lt; 1.2 , gevsq the elastic process and 0t| &lt; 8 , gevsq proton dissociation. The results are compared to other measurements. The Wgp 0dependences are parametrised using phenomenological fits.
DOI: 10.17182/hepdata.66507.v1/t7
title: "Table 7" of "Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA"

description: The elastic photoproduction differential cross section derived from the low-energy data set as a function of the negative squared momentum transfer at the proton vertex T.
description: DESY-HERA. Cross sections for elastic and proton-dissociative photoproduction of J/psi mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at -of-mass energies sqrt{s} approx 318 GeV and sqrt{s} approx 225 GeV, corresponding to integrated luminosities of L = 130 pb^{-1} and L = 10.8 pb^{-1}, respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25&lt; Wgp &lt; 110 GeV. Differential cross sections mathrm{d}sigma / mathrm{d}t where the squared four-momentum transfer at the proton vertex, are measured in the range 0t| &lt; 1.2 , gevsq the elastic process and 0t| &lt; 8 , gevsq proton dissociation. The results are compared to other measurements. The Wgp 0dependences are parametrised using phenomenological fits.
DOI: 10.17182/hepdata.66507.v1/t8
title: "Table 8" of "Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA"

description: The proton-dissociative photoproduction differential cross section derived from the low-energy data set as a function of the negative squared momentum transfer at the proton vertex T.
description: DESY-HERA. Cross sections for elastic and proton-dissociative photoproduction of J/psi mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at -of-mass energies sqrt{s} approx 318 GeV and sqrt{s} approx 225 GeV, corresponding to integrated luminosities of L = 130 pb^{-1} and L = 10.8 pb^{-1}, respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25&lt; Wgp &lt; 110 GeV. Differential cross sections mathrm{d}sigma / mathrm{d}t where the squared four-momentum transfer at the proton vertex, are measured in the range 0t| &lt; 1.2 , gevsq the elastic process and 0t| &lt; 8 , gevsq proton dissociation. The results are compared to other measurements. The Wgp 0dependences are parametrised using phenomenological fits.
DOI: 10.17182/hepdata.66510.v1/t1
title: "Table 1" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: The measured fiducial cross section. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
description: CERN-LHC. Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pT and pseudorapidity eta, together with the correlations in azimuthal angle and the pT balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 pb-1. The cross section for exactly four jets, with two hard jets of pT&gt;50 GeV each, together with two jets of pT&gt;20 GeV each, within |eta|&lt;4.7 is measured to be sigma=330+-5(stat.)+-45(syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.

The four-jet fiducial region is defined as:
- exactly four jets in the final state in |eta|&lt;4.7.
- Two jets are required with pT &gt; 50 GeV
- Two additional jets are required with pT &gt; 20 GeV.
DOI: 10.17182/hepdata.66510.v1/t2
title: "Table 2" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: Differential cross section as a function of the transverse momentum PT of the leading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
description: CERN-LHC. Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pT and pseudorapidity eta, together with the correlations in azimuthal angle and the pT balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 pb-1. The cross section for exactly four jets, with two hard jets of pT&gt;50 GeV each, together with two jets of pT&gt;20 GeV each, within |eta|&lt;4.7 is measured to be sigma=330+-5(stat.)+-45(syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.

The four-jet fiducial region is defined as:
- exactly four jets in the final state in |eta|&lt;4.7.
- Two jets are required with pT &gt; 50 GeV
- Two additional jets are required with pT &gt; 20 GeV.
DOI: 10.17182/hepdata.66510.v1/t3
title: "Table 3" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: Differential cross section as a function of the transverse momentum PT of the subleading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
description: CERN-LHC. Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pT and pseudorapidity eta, together with the correlations in azimuthal angle and the pT balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 pb-1. The cross section for exactly four jets, with two hard jets of pT&gt;50 GeV each, together with two jets of pT&gt;20 GeV each, within |eta|&lt;4.7 is measured to be sigma=330+-5(stat.)+-45(syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.

The four-jet fiducial region is defined as:
- exactly four jets in the final state in |eta|&lt;4.7.
- Two jets are required with pT &gt; 50 GeV
- Two additional jets are required with pT &gt; 20 GeV.
DOI: 10.17182/hepdata.66510.v1/t4
title: "Table 4" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: Differential cross section as a function of the transverse momentum PT of the third jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
description: CERN-LHC. Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pT and pseudorapidity eta, together with the correlations in azimuthal angle and the pT balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 pb-1. The cross section for exactly four jets, with two hard jets of pT&gt;50 GeV each, together with two jets of pT&gt;20 GeV each, within |eta|&lt;4.7 is measured to be sigma=330+-5(stat.)+-45(syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.

The four-jet fiducial region is defined as:
- exactly four jets in the final state in |eta|&lt;4.7.
- Two jets are required with pT &gt; 50 GeV
- Two additional jets are required with pT &gt; 20 GeV.
DOI: 10.17182/hepdata.66510.v1/t5
title: "Table 5" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: Differential cross section as a function of the transverse momentum PT of the fourth jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
description: CERN-LHC. Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pT and pseudorapidity eta, together with the correlations in azimuthal angle and the pT balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 pb-1. The cross section for exactly four jets, with two hard jets of pT&gt;50 GeV each, together with two jets of pT&gt;20 GeV each, within |eta|&lt;4.7 is measured to be sigma=330+-5(stat.)+-45(syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.

The four-jet fiducial region is defined as:
- exactly four jets in the final state in |eta|&lt;4.7.
- Two jets are required with pT &gt; 50 GeV
- Two additional jets are required with pT &gt; 20 GeV.
DOI: 10.17182/hepdata.66510.v1/t6
title: "Table 6" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: Differential cross section as a function of the pseudorapidity eta of the leading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
description: CERN-LHC. Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pT and pseudorapidity eta, together with the correlations in azimuthal angle and the pT balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 pb-1. The cross section for exactly four jets, with two hard jets of pT&gt;50 GeV each, together with two jets of pT&gt;20 GeV each, within |eta|&lt;4.7 is measured to be sigma=330+-5(stat.)+-45(syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.

The four-jet fiducial region is defined as:
- exactly four jets in the final state in |eta|&lt;4.7.
- Two jets are required with pT &gt; 50 GeV
- Two additional jets are required with pT &gt; 20 GeV.
DOI: 10.17182/hepdata.66510.v1/t7
title: "Table 7" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: Differential cross section as a function of the pseudorapidity eta of the subleading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
description: CERN-LHC. Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pT and pseudorapidity eta, together with the correlations in azimuthal angle and the pT balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 pb-1. The cross section for exactly four jets, with two hard jets of pT&gt;50 GeV each, together with two jets of pT&gt;20 GeV each, within |eta|&lt;4.7 is measured to be sigma=330+-5(stat.)+-45(syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.

The four-jet fiducial region is defined as:
- exactly four jets in the final state in |eta|&lt;4.7.
- Two jets are required with pT &gt; 50 GeV
- Two additional jets are required with pT &gt; 20 GeV.
DOI: 10.17182/hepdata.66510.v1/t10
title: "Table 10" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: Differential cross section as a function of the azimuthal angle DeltaPhi between the third and the fourth jet, normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
description: CERN-LHC. Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pT and pseudorapidity eta, together with the correlations in azimuthal angle and the pT balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 pb-1. The cross section for exactly four jets, with two hard jets of pT&gt;50 GeV each, together with two jets of pT&gt;20 GeV each, within |eta|&lt;4.7 is measured to be sigma=330+-5(stat.)+-45(syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.

The four-jet fiducial region is defined as:
- exactly four jets in the final state in |eta|&lt;4.7.
- Two jets are required with pT &gt; 50 GeV
- Two additional jets are required with pT &gt; 20 GeV.