cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.69366.v1/t91
title: "Table 91" of "ATLAS Run 1 searches for direct pair production of third-generation squarks at the Large Hadron Collider"

description: 95% CL exclusion limits for the pMSSM model with well-tempered neutralinos as a function of M1 and mqL3. The limit is obtained as the combination of the t0L, t1L, tb and SS3L analyses, This table is for the best expected signal region.
description: CERN-LHC. This paper reviews and extends searches for the direct pair production of the scalar supersymmetric partners of the top and bottom quarks in proton--proton collisions collected by the ATLAS collaboration during the LHC Run 1. Most of the analyses use 20 fb$^{-1}$ of collisions at a centre-of-mass energy of $\sqrt{s} = 8$ TeV, although in some case an additional 4.7 fb$^{-1}$ of collision data at $\sqrt{s}= 7$ TeV are used. New analyses are introduced to improve the sensitivity to specific regions of the model parameter space. Since no evidence of third-generation squarks is found, exclusion limits are derived by combining several analyses and are presented in both a simplified model framework, assuming simple decay chains, as well as within the context of more elaborate phenomenological supersymmetric models.
DOI: 10.17182/hepdata.69366.v1/t92
title: "Table 92" of "ATLAS Run 1 searches for direct pair production of third-generation squarks at the Large Hadron Collider"

description: Expected 95% CL exclusion limits for the pMSSM model with well-tempered neutralinos as a function of M1 and mtR. The limit is obtained using the t0L analysis. This table is for the best expected signal region.
description: CERN-LHC. This paper reviews and extends searches for the direct pair production of the scalar supersymmetric partners of the top and bottom quarks in proton--proton collisions collected by the ATLAS collaboration during the LHC Run 1. Most of the analyses use 20 fb$^{-1}$ of collisions at a centre-of-mass energy of $\sqrt{s} = 8$ TeV, although in some case an additional 4.7 fb$^{-1}$ of collision data at $\sqrt{s}= 7$ TeV are used. New analyses are introduced to improve the sensitivity to specific regions of the model parameter space. Since no evidence of third-generation squarks is found, exclusion limits are derived by combining several analyses and are presented in both a simplified model framework, assuming simple decay chains, as well as within the context of more elaborate phenomenological supersymmetric models.
DOI: 10.17182/hepdata.69366.v1/t93
title: "Table 93" of "ATLAS Run 1 searches for direct pair production of third-generation squarks at the Large Hadron Collider"

description: 95% CL exclusion limits for the set of h/Z-enriched pMSSM models as a function of $\mu$ and m(qL3). The limit of is obtained as the combination of the t0L, g3b, t2t1Z and SS3L analyses, This table is for the best expected signal region.
description: CERN-LHC. This paper reviews and extends searches for the direct pair production of the scalar supersymmetric partners of the top and bottom quarks in proton--proton collisions collected by the ATLAS collaboration during the LHC Run 1. Most of the analyses use 20 fb$^{-1}$ of collisions at a centre-of-mass energy of $\sqrt{s} = 8$ TeV, although in some case an additional 4.7 fb$^{-1}$ of collision data at $\sqrt{s}= 7$ TeV are used. New analyses are introduced to improve the sensitivity to specific regions of the model parameter space. Since no evidence of third-generation squarks is found, exclusion limits are derived by combining several analyses and are presented in both a simplified model framework, assuming simple decay chains, as well as within the context of more elaborate phenomenological supersymmetric models.
DOI: 10.17182/hepdata.69366.v1/t94
title: "Table 94" of "ATLAS Run 1 searches for direct pair production of third-generation squarks at the Large Hadron Collider"

description: 95% CL exclusion limits for the set of h/Z-enriched pMSSM models as a function of $\mu$ and m(bR). The limit of is obtained as the combination of the t0L, t2t1Z and tb analyses, This table is for the best expected signal region.
description: CERN-LHC. This paper reviews and extends searches for the direct pair production of the scalar supersymmetric partners of the top and bottom quarks in proton--proton collisions collected by the ATLAS collaboration during the LHC Run 1. Most of the analyses use 20 fb$^{-1}$ of collisions at a centre-of-mass energy of $\sqrt{s} = 8$ TeV, although in some case an additional 4.7 fb$^{-1}$ of collision data at $\sqrt{s}= 7$ TeV are used. New analyses are introduced to improve the sensitivity to specific regions of the model parameter space. Since no evidence of third-generation squarks is found, exclusion limits are derived by combining several analyses and are presented in both a simplified model framework, assuming simple decay chains, as well as within the context of more elaborate phenomenological supersymmetric models.
DOI: 10.17182/hepdata.69375.v1/t1
title: "Table 1" of "Pseudorapidity distribution of charged hadrons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of the pseudorapidity density of charged hadrons in the region $|\eta|&lt;2$ in inelastic pp collisions are 13 TeV.
description: The pseudorapidity distribution of charged hadrons in pp collisions at sqrt(s) =13 TeV is measured using a data sample obtained with the CMS detector, operated at zero magnetic field, at the CERN LHC. The yield of primary charged long-lived hadrons produced in inelastic pp collisions is determined in the central region of the CMS pixel detector (abs(eta)&lt;2) using both hit pairs and reconstructed tracks. For central pseudorapidities (abs(eta)&lt;0.5), the charged-hadron multiplicity density is dN/d(eta)[charged,abs(eta) &lt; 0.5] = 5.49 +/- 0.01 (stat) +/- 0.17 (sys), a value obtained by combining the two methods. The result is compared to predictions from Monte Carlo event generators and to similar measurements made at lower collision energies.
DOI: 10.17182/hepdata.69471.v1/t1
title: "Table 1" of "Measurement of the $K_L$ nuclear interaction length in the NaI(Tl) calorimeter"

description: The energy interval ($\sqrt{s}$), integrated luminosity ($IL$), number of selected events ($N$), number of background events ($N_{\rm bkg}$), number of events with five or more photons ($N_{5\gamma}$, $N_{5\gamma,{\rm bkg}}$), and the measured $K_L$ nuclear interaction length in NaI(Tl) ($\lambda_{\rm int}$).
description: NOVOSIBIRSK-VEPP-2M. In the study of the reaction $e^+e^-\to K_{S}K_{L}$ at the VEPP-2M $e^+e^-$ collider with the SND detector the nuclear interaction length of $K_{L}$ meson in NaI(Tl) has been measured. Its value is found to be 30-50 cm in the $K_{L}$ momentum range 0.11-0.48 GeV/$c$. The results are compared with the values used in the simulation programs GEANT4 and UNIMOD.
DOI: 10.17182/hepdata.69473.v1/t1
title: "Table 1" of "Measurement of Higgs boson production in the diphoton decay channel in $pp$ collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector"

description: The signal strength for a Higgs boson of mass mH = 125.4 GeV decaying via H-&gt;gammagamma as measured in the individual analysis categories, and the combined signal strength, for the combination of the 7 TeV and 8 TeV data. The VH dilepton category is not shown because with only two events in the combined sample, the fit results are not meaningful.
description: A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 5.4 fb-1 of proton-proton collisions data at sqrt(s)=7 TeV and 20.3 fb-1 at sqrt(s)=8 TeV collected by the ATLAS detector at the Large Hadron Collider.
DOI: 10.17182/hepdata.69473.v1/t2
title: "Table 2" of "Measurement of Higgs boson production in the diphoton decay channel in $pp$ collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector"

description: The signal strength for a Higgs boson of mass mH = 125.4 GeV decaying via H-&gt;gammagamma as measured in groups of categories sensitive to individual production modes, and the combined signal strength, for the combination of the 7 TeV and 8 TeV data.
description: A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 5.4 fb-1 of proton-proton collisions data at sqrt(s)=7 TeV and 20.3 fb-1 at sqrt(s)=8 TeV collected by the ATLAS detector at the Large Hadron Collider.
DOI: 10.17182/hepdata.69473.v1/t3
title: "Table 3" of "Measurement of Higgs boson production in the diphoton decay channel in $pp$ collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector"

description: Measured signal strengths, for a Higgs boson of mass mH = 125.4 GeV decaying via H-&gt;gammagamma, of the different Higgs boson production modes and the combined signal strength mu obtained with the combination of the 7 TeV and 8 TeV data.
description: A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 5.4 fb-1 of proton-proton collisions data at sqrt(s)=7 TeV and 20.3 fb-1 at sqrt(s)=8 TeV collected by the ATLAS detector at the Large Hadron Collider.
DOI: 10.17182/hepdata.69477.v1/t1
title: "Table 1" of "Measurement of dijet $\mathbf{{\textit{k}}_{T}}$ in p-Pb collisions at $\mathbf{\sqrt{{\textit{s}}_{NN}}=5.02}$ TeV"

description: Dijet |k_{T,y}| distributions in p-Pb collisions in the 0-40% V0A multiplicity event class.
description: CERN-LHC. 
A measurement of dijet correlations in p-Pb collisions at $\mathbf{\sqrt{{\it s}_{NN}}}=5.02$ TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. 
A projection of the dijet transverse momentum, $\it{k}_{T,y} = p_\mathrm{T,jet}^\mathrm{ch+ne} \; \mathrm{sin}(\Delta \phi_{\mathrm{dijet}})$ with $\Delta \phi_{\mathrm{dijet}}$ the azimuthal angle between a full and charged jet and $p_\mathrm{T,jet}^\mathrm{ch+ne}$ the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet $\it{k}_{T,y}$ as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of $\it{k}_{T,y}$ due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed.
DOI: 10.17182/hepdata.69477.v1/t2
title: "Table 2" of "Measurement of dijet $\mathbf{{\textit{k}}_{T}}$ in p-Pb collisions at $\mathbf{\sqrt{{\textit{s}}_{NN}}=5.02}$ TeV"

description: Dijet |k_{T,y}| distributions in p-Pb collisions in the 0-40% V0A multiplicity event class.
description: CERN-LHC. 
A measurement of dijet correlations in p-Pb collisions at $\mathbf{\sqrt{{\it s}_{NN}}}=5.02$ TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. 
A projection of the dijet transverse momentum, $\it{k}_{T,y} = p_\mathrm{T,jet}^\mathrm{ch+ne} \; \mathrm{sin}(\Delta \phi_{\mathrm{dijet}})$ with $\Delta \phi_{\mathrm{dijet}}$ the azimuthal angle between a full and charged jet and $p_\mathrm{T,jet}^\mathrm{ch+ne}$ the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet $\it{k}_{T,y}$ as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of $\it{k}_{T,y}$ due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed.
DOI: 10.17182/hepdata.69477.v1/t3
title: "Table 3" of "Measurement of dijet $\mathbf{{\textit{k}}_{T}}$ in p-Pb collisions at $\mathbf{\sqrt{{\textit{s}}_{NN}}=5.02}$ TeV"

description: Dijet |k_{T,y}| distributions in p-Pb collisions in the 0-40% V0A multiplicity event class.
description: CERN-LHC. 
A measurement of dijet correlations in p-Pb collisions at $\mathbf{\sqrt{{\it s}_{NN}}}=5.02$ TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. 
A projection of the dijet transverse momentum, $\it{k}_{T,y} = p_\mathrm{T,jet}^\mathrm{ch+ne} \; \mathrm{sin}(\Delta \phi_{\mathrm{dijet}})$ with $\Delta \phi_{\mathrm{dijet}}$ the azimuthal angle between a full and charged jet and $p_\mathrm{T,jet}^\mathrm{ch+ne}$ the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet $\it{k}_{T,y}$ as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of $\it{k}_{T,y}$ due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed.
DOI: 10.17182/hepdata.69477.v1/t4
title: "Table 4" of "Measurement of dijet $\mathbf{{\textit{k}}_{T}}$ in p-Pb collisions at $\mathbf{\sqrt{{\textit{s}}_{NN}}=5.02}$ TeV"

description: Dijet |k_{T,y}| distributions in p-Pb collisions in the 0-40% V0A multiplicity event class.
description: CERN-LHC. 
A measurement of dijet correlations in p-Pb collisions at $\mathbf{\sqrt{{\it s}_{NN}}}=5.02$ TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. 
A projection of the dijet transverse momentum, $\it{k}_{T,y} = p_\mathrm{T,jet}^\mathrm{ch+ne} \; \mathrm{sin}(\Delta \phi_{\mathrm{dijet}})$ with $\Delta \phi_{\mathrm{dijet}}$ the azimuthal angle between a full and charged jet and $p_\mathrm{T,jet}^\mathrm{ch+ne}$ the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet $\it{k}_{T,y}$ as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of $\it{k}_{T,y}$ due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed.
DOI: 10.17182/hepdata.69477.v1/t5
title: "Table 5" of "Measurement of dijet $\mathbf{{\textit{k}}_{T}}$ in p-Pb collisions at $\mathbf{\sqrt{{\textit{s}}_{NN}}=5.02}$ TeV"

description: Dijet |k_{T,y}| distributions in p-Pb collisions in the 40-100% V0A multiplicity event class.
description: CERN-LHC. 
A measurement of dijet correlations in p-Pb collisions at $\mathbf{\sqrt{{\it s}_{NN}}}=5.02$ TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. 
A projection of the dijet transverse momentum, $\it{k}_{T,y} = p_\mathrm{T,jet}^\mathrm{ch+ne} \; \mathrm{sin}(\Delta \phi_{\mathrm{dijet}})$ with $\Delta \phi_{\mathrm{dijet}}$ the azimuthal angle between a full and charged jet and $p_\mathrm{T,jet}^\mathrm{ch+ne}$ the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet $\it{k}_{T,y}$ as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of $\it{k}_{T,y}$ due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed.
DOI: 10.17182/hepdata.69477.v1/t6
title: "Table 6" of "Measurement of dijet $\mathbf{{\textit{k}}_{T}}$ in p-Pb collisions at $\mathbf{\sqrt{{\textit{s}}_{NN}}=5.02}$ TeV"

description: Dijet |k_{T,y}| distributions in p-Pb collisions in the 0-40% V0A multiplicity event class.
description: CERN-LHC. 
A measurement of dijet correlations in p-Pb collisions at $\mathbf{\sqrt{{\it s}_{NN}}}=5.02$ TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. 
A projection of the dijet transverse momentum, $\it{k}_{T,y} = p_\mathrm{T,jet}^\mathrm{ch+ne} \; \mathrm{sin}(\Delta \phi_{\mathrm{dijet}})$ with $\Delta \phi_{\mathrm{dijet}}$ the azimuthal angle between a full and charged jet and $p_\mathrm{T,jet}^\mathrm{ch+ne}$ the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet $\it{k}_{T,y}$ as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of $\it{k}_{T,y}$ due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed.
DOI: 10.17182/hepdata.69477.v1/t7
title: "Table 7" of "Measurement of dijet $\mathbf{{\textit{k}}_{T}}$ in p-Pb collisions at $\mathbf{\sqrt{{\textit{s}}_{NN}}=5.02}$ TeV"

description: Dijet |k_{T,y}| distributions in p-Pb collisions in the 0-40% V0A multiplicity event class.
description: CERN-LHC. 
A measurement of dijet correlations in p-Pb collisions at $\mathbf{\sqrt{{\it s}_{NN}}}=5.02$ TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. 
A projection of the dijet transverse momentum, $\it{k}_{T,y} = p_\mathrm{T,jet}^\mathrm{ch+ne} \; \mathrm{sin}(\Delta \phi_{\mathrm{dijet}})$ with $\Delta \phi_{\mathrm{dijet}}$ the azimuthal angle between a full and charged jet and $p_\mathrm{T,jet}^\mathrm{ch+ne}$ the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet $\it{k}_{T,y}$ as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of $\it{k}_{T,y}$ due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed.
DOI: 10.17182/hepdata.69477.v1/t8
title: "Table 8" of "Measurement of dijet $\mathbf{{\textit{k}}_{T}}$ in p-Pb collisions at $\mathbf{\sqrt{{\textit{s}}_{NN}}=5.02}$ TeV"

description: Dijet |k_{T,y}| distributions in p-Pb collisions in the 0-40% V0A multiplicity event class.
description: CERN-LHC. 
A measurement of dijet correlations in p-Pb collisions at $\mathbf{\sqrt{{\it s}_{NN}}}=5.02$ TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. 
A projection of the dijet transverse momentum, $\it{k}_{T,y} = p_\mathrm{T,jet}^\mathrm{ch+ne} \; \mathrm{sin}(\Delta \phi_{\mathrm{dijet}})$ with $\Delta \phi_{\mathrm{dijet}}$ the azimuthal angle between a full and charged jet and $p_\mathrm{T,jet}^\mathrm{ch+ne}$ the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet $\it{k}_{T,y}$ as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of $\it{k}_{T,y}$ due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed.