cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.66510.v1/t11
title: "Table 11" of "Measurement of four-jet production in proton-proton collisions at sqrt(s)=7 TeV"

description: Differential cross section as a function of the normalized PT balance DELTARELPT 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.
DOI: 10.17182/hepdata.66510.v1/t12
title: "Table 12" 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 between the two dijet planes (first-second and third-fourth jets), 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.
DOI: 10.17182/hepdata.66510.v1/t8
title: "Table 8" 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 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/t9
title: "Table 9" 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 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.66529.v1/t1
title: "Table 1" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The cross section ratios B.R. sigma_Psi(2S)/ B.R. sigma_JPsi obtained in p-Pb and Pb-p collisions. 
The first uncertainty is statistical, the second one is systematic.
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66529.v1/t2
title: "Table 2" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The double ratio [sigma(Psi(2S))/sigma(J/Psi)]_pA/[sigma(Psi(2S))/sigma(J/Psi)]_pp for p-Pb and Pb-p collisions.
First uncertainty is statistical, the second one is the correlated systematic, while the third is the uncorrelated systematic.
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66529.v1/t3
title: "Table 3" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Psi(2S) nuclear modification factor RpA measured in pPb and Pbp collisions. 
The first uncertainty is statistical, the second one is the correlated systematic and the third the uncorrelated systematic.
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66529.v1/t4
title: "Table 4" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Psi(2S) pT-differential cross sections in p-Pb, in the centre of mass rapidity range 2.03
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66529.v1/t5
title: "Table 5" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Psi(2S) pT-differential cross sections in Pb-p, in the centre of mass rapidity range -4.46
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66529.v1/t6
title: "Table 6" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Double ratio [sigma(Psi(2S))/sigma(J/Psi)]_pA/[sigma(Psi(2S))/sigma(J/Psi)]_pp in p-Pb collisions as a function of pT. 
Results are obtained in the centre of mass rapidity range 2.03
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66529.v1/t7
title: "Table 7" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Double ratio [sigma(Psi(2S))/sigma(J/Psi)]_pA/[sigma(Psi(2S))/sigma(J/Psi)]_pp in Pb-p collisions as a function of pT. 
Results are obtained in the centre of mass rapidity range -4.46
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66529.v1/t8
title: "Table 8" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Psi(2S) RpA versus pT in p-Pb collisions.
Results are obtained in the centre of mass rapidity range 2.03
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66529.v1/t9
title: "Table 9" of "Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Psi(2S) RpA versus pT in Pb-p collisions.
Results are obtained in the centre of mass rapidity range -4.46
description: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03
DOI: 10.17182/hepdata.66539.v1/t1
title: "Table 1" of "Search for resonant diboson production in the $\ell\ell q\bar{q}$ final state in pp collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector"

description: 1D histogram with combined statistical and systematic errors representing the event yields as a function of the reconstructed
M(lljj) for the LR (low-pt resolved signal region) and HR (high-pt resolved signal region) and M(llJ) for the MR (merged signal region).
system. The value of mass on the x axis is given for the lower edge of the bin.
description: CERN-LHC. This paper reports on a search for narrow resonances in diboson production in the $\ell\ell q\bar{q}$ final state using pp collision data corresponding to an integrated luminosity of 20 fb$^{-1}$ collected at $;sqrt{s}=8$ TeV with the ATLAS detector at the Large Hadron Collider. No significant excess of data events over the Standard Model expectation is observed. Upper limits at the 95% confidence level are set on the production cross section times branching ratio for Kaluza--Klein gravitons predicted by the Randall--Sundrum model and for Extended Gauge Model W' bosons. These results lead to the exclusion of mass values below 740 GeV and 1590 GeV for the graviton and W' boson respectively.
DOI: 10.17182/hepdata.66539.v1/t2
title: "Table 2" of "Search for resonant diboson production in the $\ell\ell q\bar{q}$ final state in pp collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector"

description: The theoretical cross section, the expected upper limit, and observed upper limit for the Kaluza Klein graviton signal mass points studied.
description: CERN-LHC. This paper reports on a search for narrow resonances in diboson production in the $\ell\ell q\bar{q}$ final state using pp collision data corresponding to an integrated luminosity of 20 fb$^{-1}$ collected at $;sqrt{s}=8$ TeV with the ATLAS detector at the Large Hadron Collider. No significant excess of data events over the Standard Model expectation is observed. Upper limits at the 95% confidence level are set on the production cross section times branching ratio for Kaluza--Klein gravitons predicted by the Randall--Sundrum model and for Extended Gauge Model W' bosons. These results lead to the exclusion of mass values below 740 GeV and 1590 GeV for the graviton and W' boson respectively.
DOI: 10.17182/hepdata.66539.v1/t3
title: "Table 3" of "Search for resonant diboson production in the $\ell\ell q\bar{q}$ final state in pp collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector"

description: The theoretical cross section, the expected upper limit, and observed upper limit for the SSM W-prime signal mass point studied.
description: CERN-LHC. This paper reports on a search for narrow resonances in diboson production in the $\ell\ell q\bar{q}$ final state using pp collision data corresponding to an integrated luminosity of 20 fb$^{-1}$ collected at $;sqrt{s}=8$ TeV with the ATLAS detector at the Large Hadron Collider. No significant excess of data events over the Standard Model expectation is observed. Upper limits at the 95% confidence level are set on the production cross section times branching ratio for Kaluza--Klein gravitons predicted by the Randall--Sundrum model and for Extended Gauge Model W' bosons. These results lead to the exclusion of mass values below 740 GeV and 1590 GeV for the graviton and W' boson respectively.
DOI: 10.17182/hepdata.66543.v1/t1
title: "Table 1" of "Measurement of the combined rapidity and $p_T$ dependence of dijet azimuthal decorrelations in $p\bar{p}$ collisions at $\sqrt{s}=1.96\,$TeV"

description: The results for $R_{\Delta\phi}$ with their relative uncertainties for $\Delta\phi_{\rm max}=7\pi/8$.
description: FNAL-D0. We present the first combined measurement of the rapidity and transverse momentum dependence of dijet azimuthal decorrelations, based on the recently proposed quantity $R_{\Delta \phi}$. The variable $R_{\Delta \phi}$ measures the fraction of the inclusive dijet events in which the azimuthal separation of the two jets with the highest transverse momenta is less than a specified value for the parameter $\Delta \phi_{\rm max}$. The quantity $R_{\Delta \phi}$ is measured in $p\bar{p}$ collisions at $\sqrt{s}=1.96\,$TeV, as a function of the dijet rapidity interval, the total scalar transverse momentum, and $\Delta \phi_{\rm max}$. The measurement uses an event sample corresponding to an integrated luminosity of $0.7\,$fb$^{-1}$ collected with the D0 detector at the Fermilab Tevatron Collider. The results are compared to predictions of a perturbative QCD calculation at next-to-leading order in the strong coupling with corrections for non-perturbative effects. The theory predictions describe the data, except in the kinematic region of large dijet rapidity intervals and large $\Delta \phi_{\rm max}$.
DOI: 10.17182/hepdata.66543.v1/t2
title: "Table 2" of "Measurement of the combined rapidity and $p_T$ dependence of dijet azimuthal decorrelations in $p\bar{p}$ collisions at $\sqrt{s}=1.96\,$TeV"

description: The results for $R_{\delta\phi}$ with their relative uncertainties for $\delta\phi_{\rm max}=5\pi/6$.
description: FNAL-D0. We present the first combined measurement of the rapidity and transverse momentum dependence of dijet azimuthal decorrelations, based on the recently proposed quantity $R_{\Delta \phi}$. The variable $R_{\Delta \phi}$ measures the fraction of the inclusive dijet events in which the azimuthal separation of the two jets with the highest transverse momenta is less than a specified value for the parameter $\Delta \phi_{\rm max}$. The quantity $R_{\Delta \phi}$ is measured in $p\bar{p}$ collisions at $\sqrt{s}=1.96\,$TeV, as a function of the dijet rapidity interval, the total scalar transverse momentum, and $\Delta \phi_{\rm max}$. The measurement uses an event sample corresponding to an integrated luminosity of $0.7\,$fb$^{-1}$ collected with the D0 detector at the Fermilab Tevatron Collider. The results are compared to predictions of a perturbative QCD calculation at next-to-leading order in the strong coupling with corrections for non-perturbative effects. The theory predictions describe the data, except in the kinematic region of large dijet rapidity intervals and large $\Delta \phi_{\rm max}$.
DOI: 10.17182/hepdata.66543.v1/t3
title: "Table 3" of "Measurement of the combined rapidity and $p_T$ dependence of dijet azimuthal decorrelations in $p\bar{p}$ collisions at $\sqrt{s}=1.96\,$TeV"

description: The results for $R_{\delta\phi}$ with their relative uncertainties for $\delta\phi_{\rm max}=3\pi/4$.
description: FNAL-D0. We present the first combined measurement of the rapidity and transverse momentum dependence of dijet azimuthal decorrelations, based on the recently proposed quantity $R_{\Delta \phi}$. The variable $R_{\Delta \phi}$ measures the fraction of the inclusive dijet events in which the azimuthal separation of the two jets with the highest transverse momenta is less than a specified value for the parameter $\Delta \phi_{\rm max}$. The quantity $R_{\Delta \phi}$ is measured in $p\bar{p}$ collisions at $\sqrt{s}=1.96\,$TeV, as a function of the dijet rapidity interval, the total scalar transverse momentum, and $\Delta \phi_{\rm max}$. The measurement uses an event sample corresponding to an integrated luminosity of $0.7\,$fb$^{-1}$ collected with the D0 detector at the Fermilab Tevatron Collider. The results are compared to predictions of a perturbative QCD calculation at next-to-leading order in the strong coupling with corrections for non-perturbative effects. The theory predictions describe the data, except in the kinematic region of large dijet rapidity intervals and large $\Delta \phi_{\rm max}$.
DOI: 10.17182/hepdata.66547.v1/t1
title: "Table 1" of "Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector"

description: Transverse polarization POL of LAMBDA and LAMBDABAR hyperons averaged over PT and XF.
description: CERN-LHC. The transverse polarization of LAMBDA and LAMBDABAR hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses $760 \mu{}b^{-1}$ of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from $5 \times 10^{-5}$ to 0.01 and transverse momentum pT from 0.8 to 15 GeV is $-0.010 \pm 0.005(stat) \pm 0.004(syst)$ for LAMBDA and $0.002 \pm 0.006(stat) \pm 0.004(syst)$ for LAMBDABAR. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement.
DOI: 10.17182/hepdata.66547.v1/t2
title: "Table 2" of "Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector"

description: Transverse polarization POL of LAMBDA and LAMBDABAR hyperons as a function of XF.
description: CERN-LHC. The transverse polarization of LAMBDA and LAMBDABAR hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses $760 \mu{}b^{-1}$ of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from $5 \times 10^{-5}$ to 0.01 and transverse momentum pT from 0.8 to 15 GeV is $-0.010 \pm 0.005(stat) \pm 0.004(syst)$ for LAMBDA and $0.002 \pm 0.006(stat) \pm 0.004(syst)$ for LAMBDABAR. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement.
DOI: 10.17182/hepdata.66547.v1/t3
title: "Table 3" of "Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector"

description: Transverse polarization POL of LAMBDA and LAMBDABAR hyperons as a function of PT.
description: CERN-LHC. The transverse polarization of LAMBDA and LAMBDABAR hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses $760 \mu{}b^{-1}$ of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from $5 \times 10^{-5}$ to 0.01 and transverse momentum pT from 0.8 to 15 GeV is $-0.010 \pm 0.005(stat) \pm 0.004(syst)$ for LAMBDA and $0.002 \pm 0.006(stat) \pm 0.004(syst)$ for LAMBDABAR. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement.
DOI: 10.17182/hepdata.66547.v1/t4
title: "Table 4" of "Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector"

description: The LAMBDA reconstruction and selection efficiency EFF as a function of PT and XF.
description: CERN-LHC. The transverse polarization of LAMBDA and LAMBDABAR hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses $760 \mu{}b^{-1}$ of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from $5 \times 10^{-5}$ to 0.01 and transverse momentum pT from 0.8 to 15 GeV is $-0.010 \pm 0.005(stat) \pm 0.004(syst)$ for LAMBDA and $0.002 \pm 0.006(stat) \pm 0.004(syst)$ for LAMBDABAR. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement.