cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.65525.v1/t113
title: "Table 113" of "Search for supersymmetry in events with large missing transverse momentum, jets, and at least one tau lepton in 20 fb$^{-1}$ of $\sqrt{s}$=8 TeV proton-proton collision data with the ATLAS detector"

description: Example cutflow for four benchmark signal points in the tau+mu analysis. Event numbers are normalised to 21 fb^{-1} luminosity. For the GMSB point 50000 events have been generated, 20000 for nGM, 20000 for mSUGRA and 25000 for bRPV respectively.
description: CERN-LHC. A search for supersymmetry (SUSY) in events with large missing transverse momentum, jets, at least one hadronically decaying tau lepton and zero or one additional light leptons (electron/muon), has been performed using 20.3 fb^-1 of proton-proton collision data at sqrt(s)=8 TeV recorded with the ATLAS detector at the Large Hadron Collider. No excess above the Standard Model background expectation is observed in the various signal regions and 95% confidence level upper limits on the visible cross section for new phenomena are set. The results of the analysis are interpreted in several SUSY scenarios, significantly extending previous limits obtained in the same final states. In the framework of minimal gauge-mediated SUSY breaking models, values of the SUSY breaking scale Lambda below 63 TeV are excluded, independently of tan(beta). Exclusion limits are also derived for an mSUGRA/CMSSM model, in both the R-parity-conserving and R-parity-violating case. A further interpretation is presented in a framework of natural gauge mediation, in which the gluino is assumed to be the only light coloured sparticle and gluino masses below 1090 GeV are excluded.
DOI: 10.17182/hepdata.65545.v1/t1
title: "Table 1" of "Measurement of the cross-section for Z-&gt;e+e- production in pp collisions at sqrt{s}=7TeV"

description: Cross-section of $pp \to Z \to e^+ e^-$ integrated over $Z$ rapidity. The first quoted uncertainty is statistical, the second is the experimental systematic uncertainty, the third is the luminosity uncertainty and the fourth uncertainty is due to FSR correction.
description: CERN-LHC. Measurement of the cross-section $pp \to \mathrm{Z}^0 \to e^+ e^-$ using data at $\sqrt{s} = 7$ TeV corresponding to an integrated luminosity of 0.94 fb$^{-1}$. The process is measured within the kinematic acceptance $p_\perp &gt; 20$GeV/$c$ and $2 &lt; \eta &lt; 4.5$ for the daughter electrons and dielectron invariant mass in the range 60-120 GeV/$c^2$. The integrated cross-section is determined to be $\sigma(pp \to \mathrm{Z}^0 \to e^+ e^-) = 76.0 \pm 0.8 \pm 2.0 \pm 2.6 \pm 0.4$ pb, where the first uncertainty is statistical, the second is systematic, the third is the uncertainty in the luminosity and the fourth represents the uncertainty in the FSR correction. Differential cross-sections are measured as a function of $\mathrm{Z}^0$ rapidity and as a function of an angular variable ($\phi^*$) which is closely related to the Z$^0$ transverse momentum.
DOI: 10.17182/hepdata.65545.v1/t2
title: "Table 2" of "Measurement of the cross-section for Z-&gt;e+e- production in pp collisions at sqrt{s}=7TeV"

description: Differential cross-section of $pp \to Z \to e^+ e^-$ as function $Z$ rapidity. The first quoted uncertainty is statistical. The second and third uncertainties are the uncorrelated and correlated systematic uncertainties respectively. The fourth uncertainty is due to FSR correction.
description: CERN-LHC. Measurement of the cross-section $pp \to \mathrm{Z}^0 \to e^+ e^-$ using data at $\sqrt{s} = 7$ TeV corresponding to an integrated luminosity of 0.94 fb$^{-1}$. The process is measured within the kinematic acceptance $p_\perp &gt; 20$GeV/$c$ and $2 &lt; \eta &lt; 4.5$ for the daughter electrons and dielectron invariant mass in the range 60-120 GeV/$c^2$. The integrated cross-section is determined to be $\sigma(pp \to \mathrm{Z}^0 \to e^+ e^-) = 76.0 \pm 0.8 \pm 2.0 \pm 2.6 \pm 0.4$ pb, where the first uncertainty is statistical, the second is systematic, the third is the uncertainty in the luminosity and the fourth represents the uncertainty in the FSR correction. Differential cross-sections are measured as a function of $\mathrm{Z}^0$ rapidity and as a function of an angular variable ($\phi^*$) which is closely related to the Z$^0$ transverse momentum.
DOI: 10.17182/hepdata.65267.v1/t5
title: "Table 5" of "Rapidity distributions in exclusive Z + jet and $\gamma$ + jet events in pp collisions at $\sqrt{s}$=7 TeV"

description: Distributions of |YPho| normalized to unity. The data are shown after correcting for efficiency and resolution, and displayed with statistical and systematic uncertainties combined in quadrature.
description: CERN-LHC. Rapidity distributions are presented for events containing either a Z boson or a photon with a single jet in proton-proton collisions produced at the CERN LHC. The data, collected with the CMS detector at sqrt(s) = 7 TeV, correspond to an integrated luminosity of 5.0 fb^-1. The individual rapidity distributions of the boson and the jet are consistent within 5% with expectations from perturbative QCD. However, QCD predictions for the sum and the difference in rapidities of the two final-state objects show discrepancies with CMS data. In particular, next-to-leading-order QCD calculations, and two common Monte Carlo event generators using different methods to match matrix-element partons with parton showers, appear inconsistent with the data as well as with each other.
DOI: 10.17182/hepdata.65545.v1/t3
title: "Table 3" of "Measurement of the cross-section for Z-&gt;e+e- production in pp collisions at sqrt{s}=7TeV"

description: Differential cross-section of $pp \to Z \to e^+ e^-$ as function of $\phi^*$ kinematic variable constructed from electron pair azimuthal angle and pseudorapidity and correlated to $Z$ tranverse momentum. The first quoted uncertainty is statistical. The second and third uncertainties are the uncorrelated and correlated systematic uncertainties respectively. The fourth uncertainty is due to FSR correction.
description: CERN-LHC. Measurement of the cross-section $pp \to \mathrm{Z}^0 \to e^+ e^-$ using data at $\sqrt{s} = 7$ TeV corresponding to an integrated luminosity of 0.94 fb$^{-1}$. The process is measured within the kinematic acceptance $p_\perp &gt; 20$GeV/$c$ and $2 &lt; \eta &lt; 4.5$ for the daughter electrons and dielectron invariant mass in the range 60-120 GeV/$c^2$. The integrated cross-section is determined to be $\sigma(pp \to \mathrm{Z}^0 \to e^+ e^-) = 76.0 \pm 0.8 \pm 2.0 \pm 2.6 \pm 0.4$ pb, where the first uncertainty is statistical, the second is systematic, the third is the uncertainty in the luminosity and the fourth represents the uncertainty in the FSR correction. Differential cross-sections are measured as a function of $\mathrm{Z}^0$ rapidity and as a function of an angular variable ($\phi^*$) which is closely related to the Z$^0$ transverse momentum.
DOI: 10.17182/hepdata.65545.v1/t4
title: "Table 4" of "Measurement of the cross-section for Z-&gt;e+e- production in pp collisions at sqrt{s}=7TeV"

description: Correlation coefficients for the differential cross-section of $Z \to e^+ e^-$ at 7 TeV between bins of $Z$ rapidity, $y_{Z}$. Both statistical and systematic contributions are included.
description: CERN-LHC. Measurement of the cross-section $pp \to \mathrm{Z}^0 \to e^+ e^-$ using data at $\sqrt{s} = 7$ TeV corresponding to an integrated luminosity of 0.94 fb$^{-1}$. The process is measured within the kinematic acceptance $p_\perp &gt; 20$GeV/$c$ and $2 &lt; \eta &lt; 4.5$ for the daughter electrons and dielectron invariant mass in the range 60-120 GeV/$c^2$. The integrated cross-section is determined to be $\sigma(pp \to \mathrm{Z}^0 \to e^+ e^-) = 76.0 \pm 0.8 \pm 2.0 \pm 2.6 \pm 0.4$ pb, where the first uncertainty is statistical, the second is systematic, the third is the uncertainty in the luminosity and the fourth represents the uncertainty in the FSR correction. Differential cross-sections are measured as a function of $\mathrm{Z}^0$ rapidity and as a function of an angular variable ($\phi^*$) which is closely related to the Z$^0$ transverse momentum.
DOI: 10.17182/hepdata.65545.v1/t5
title: "Table 5" of "Measurement of the cross-section for Z-&gt;e+e- production in pp collisions at sqrt{s}=7TeV"

description: Correlation coefficients for the differential cross-section of $Z \to e^+ e^-$ at 7 TeV between bins of $\phi^*$. Both statistical and systematic contributions are included.
description: CERN-LHC. Measurement of the cross-section $pp \to \mathrm{Z}^0 \to e^+ e^-$ using data at $\sqrt{s} = 7$ TeV corresponding to an integrated luminosity of 0.94 fb$^{-1}$. The process is measured within the kinematic acceptance $p_\perp &gt; 20$GeV/$c$ and $2 &lt; \eta &lt; 4.5$ for the daughter electrons and dielectron invariant mass in the range 60-120 GeV/$c^2$. The integrated cross-section is determined to be $\sigma(pp \to \mathrm{Z}^0 \to e^+ e^-) = 76.0 \pm 0.8 \pm 2.0 \pm 2.6 \pm 0.4$ pb, where the first uncertainty is statistical, the second is systematic, the third is the uncertainty in the luminosity and the fourth represents the uncertainty in the FSR correction. Differential cross-sections are measured as a function of $\mathrm{Z}^0$ rapidity and as a function of an angular variable ($\phi^*$) which is closely related to the Z$^0$ transverse momentum.
DOI: 10.17182/hepdata.65664.v1/t1
title: "Table 1" of "Search for Top-Quark Partners with Charge 5/3 in the Same-Sign Dilepton Final State"

description: The distribution of HT for all channels combined after the full selection except for the HT requirement itself.
description: CERN-LHC. A search for the production of heavy partners of the top quark with charge 5/3 is performed in events with a pair of same-sign leptons. The data sample corresponds to an integrated luminosity of 19.5 inverse femtobarns and was collected at sqrt(s) = 8 TeV by the CMS experiment. No significant excess is observed in the data above the expected background and the existence of top-quark partners with masses below 800 GeV is excluded at a 95% confidence level, assuming they decay exclusively to tW. This is the first limit on these particles from the LHC, and it is significantly more restrictive than previous limits.
DOI: 10.17182/hepdata.65664.v1/t2
title: "Table 2" of "Search for Top-Quark Partners with Charge 5/3 in the Same-Sign Dilepton Final State"

description: Expected and observed 95% CL limits on the $\mathrm{T}_{5/3}$ production cross section times the branching fraction for decay to same-sign dileptons.
description: CERN-LHC. A search for the production of heavy partners of the top quark with charge 5/3 is performed in events with a pair of same-sign leptons. The data sample corresponds to an integrated luminosity of 19.5 inverse femtobarns and was collected at sqrt(s) = 8 TeV by the CMS experiment. No significant excess is observed in the data above the expected background and the existence of top-quark partners with masses below 800 GeV is excluded at a 95% confidence level, assuming they decay exclusively to tW. This is the first limit on these particles from the LHC, and it is significantly more restrictive than previous limits.
DOI: 10.17182/hepdata.65664.v1/t3
title: "Table 3" of "Search for Top-Quark Partners with Charge 5/3 in the Same-Sign Dilepton Final State"

description: The distribution of HT for all channels combined, after the requirement of same- sign dileptons, the Z-boson veto, and a requirement of at least two jets.
description: CERN-LHC. A search for the production of heavy partners of the top quark with charge 5/3 is performed in events with a pair of same-sign leptons. The data sample corresponds to an integrated luminosity of 19.5 inverse femtobarns and was collected at sqrt(s) = 8 TeV by the CMS experiment. No significant excess is observed in the data above the expected background and the existence of top-quark partners with masses below 800 GeV is excluded at a 95% confidence level, assuming they decay exclusively to tW. This is the first limit on these particles from the LHC, and it is significantly more restrictive than previous limits.
DOI: 10.17182/hepdata.65664.v1/t4
title: "Table 4" of "Search for Top-Quark Partners with Charge 5/3 in the Same-Sign Dilepton Final State"

description: The distribution of the reconstructed $\mathrm{T}_{5/3}$ mass for the data, the background, and three signal mass points.
description: CERN-LHC. A search for the production of heavy partners of the top quark with charge 5/3 is performed in events with a pair of same-sign leptons. The data sample corresponds to an integrated luminosity of 19.5 inverse femtobarns and was collected at sqrt(s) = 8 TeV by the CMS experiment. No significant excess is observed in the data above the expected background and the existence of top-quark partners with masses below 800 GeV is excluded at a 95% confidence level, assuming they decay exclusively to tW. This is the first limit on these particles from the LHC, and it is significantly more restrictive than previous limits.
DOI: 10.17182/hepdata.65665.v1/t1
title: "Table 1" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE0 LJs as a function of $p_{\mathrm{T}}$ of the $\gamma_{d}$ for $\gamma_{d} \to \mu\mu$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 0.4 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.
DOI: 10.17182/hepdata.65665.v1/t2
title: "Table 2" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE0 LJs as a function of $p_{\mathrm{T}}$ of the $\gamma_{d}$ for $\gamma_{d} \to \mu\mu$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 0.9 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.
DOI: 10.17182/hepdata.65665.v1/t3
title: "Table 3" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE0 LJs as a function of $p_{\mathrm{T}}$ of the $\gamma_{d}$ for $\gamma_{d} \to \mu\mu$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 1.5 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.
DOI: 10.17182/hepdata.65665.v1/t4
title: "Table 4" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE0 LJs as a function of $L_{\mathrm{xy}}$ of the $\gamma_{d}$ for $\gamma_{d} \to \mu\mu$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 0.4 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.
DOI: 10.17182/hepdata.65665.v1/t5
title: "Table 5" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE0 LJs as a function of $L_{\mathrm{xy}}$ of the $\gamma_{d}$ for $\gamma_{d} \to \mu\mu$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 0.9 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.
DOI: 10.17182/hepdata.65665.v1/t6
title: "Table 6" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE0 LJs as a function of $L_{\mathrm{xy}}$ of the $\gamma_{d}$ for $\gamma_{d} \to \mu\mu$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 1.5 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.
DOI: 10.17182/hepdata.65665.v1/t7
title: "Table 7" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE2 LJs as a function of $p_{\mathrm{T}}$ of the $\gamma_{d}$ for $\gamma_{d} \to ee,\pi\pi$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 0.05 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.
DOI: 10.17182/hepdata.65665.v1/t10
title: "Table 10" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE2 LJs as a function of $p_{\mathrm{T}}$ of the $\gamma_{d}$ for $\gamma_{d} \to ee,\pi\pi$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 0.9 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.
DOI: 10.17182/hepdata.65665.v1/t11
title: "Table 11" of "Search for long-lived neutral particles decaying into lepton jets in proton--proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Reconstruction efficiency of TYPE2 LJs as a function of $p_{\mathrm{T}}$ of the $\gamma_{d}$ for $\gamma_{d} \to ee,\pi\pi$ obtained from the LJ gun MC samples with $\gamma_{d}$ masses 1.5 GeV. The uncertainties are statistical only.
description: CERN-LHC. Several models of physics beyond the Standard Model predict neutral particles that decay into final states consisting of collimated jets of light leptons and hadrons (so-called "lepton jets"). These particles can also be long-lived with decay length comparable to, or even larger than, the LHC detectors' linear dimensions. This paper presents the results of a search for lepton jets in proton--proton collisions at the centre-of-mass energy of $\sqrt{s}$ = 8 TeV in a sample of 20.3 fb$^{-1}$ collected during 2012 with the ATLAS detector at the LHC. Limits on models predicting Higgs boson decays to neutral long-lived lepton jets are derived as a function of the particle's proper decay length.