cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64507.v1/t65
title: "Table 65" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Expected CLs for the simplified models with chargino-chargino production.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64507.v1/t66
title: "Table 66" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Expected CLs for direct stau (the left-handed) pair production.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64507.v1/t67
title: "Table 67" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Expected CLs for direct stau (the right-handed) pair production.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64597.v1/t1
title: "Table 1" of "Study of $e^+e^- \rightarrow p\bar{p}$ in the vicinity of $\psi(3770)$"

description: Summary of results at center-of-mass energies from 3.65 to 3.90 GeV. N(SIG) is the number of E+ E- --&gt; P P events; EPSILON is the detection efficiency; L is the integrated luminosity; (1 + DELTA)(DRESSED) is the initial state radiation correction factor without the vacuum polarization correction; and SIG(OBS), SIG(DRESSED) and SIG(BORN) are the observed cross section, the dressed cross section and the Born cross section, respectively.
description: BEPC-BES. Using 2917 pb^{-1} of data accumulated at 3.773 GeV, 44.5 pb^{-1} of data accumulated at 3.65 GeV and data accumulated during a PSI(3770) line-shape scan with the BESIII detector, the reaction E+ E- --&gt; P PBAR is studied considering a possible interference between resonant and continuum amplitudes. Using the obtained cross section of PSI(3770) --&gt; P PBAR, the cross section of P PBAR --&gt; PSI(3770), which is useful information for the future PANDA experiment, is estimated to be either 9.8 +- 5.7 nb (&lt; 17.2 nb at 90% C.L.) or 425.6 +- 42.9 nb.
DOI: 10.17182/hepdata.64597.v1/t2
title: "Table 2" of "Study of $e^+e^- \rightarrow p\bar{p}$ in the vicinity of $\psi(3770)$"

description: The two solutions of the dressed cross section and the corresponding phase angles, PHI.
description: BEPC-BES. Using 2917 pb^{-1} of data accumulated at 3.773 GeV, 44.5 pb^{-1} of data accumulated at 3.65 GeV and data accumulated during a PSI(3770) line-shape scan with the BESIII detector, the reaction E+ E- --&gt; P PBAR is studied considering a possible interference between resonant and continuum amplitudes. Using the obtained cross section of PSI(3770) --&gt; P PBAR, the cross section of P PBAR --&gt; PSI(3770), which is useful information for the future PANDA experiment, is estimated to be either 9.8 +- 5.7 nb (&lt; 17.2 nb at 90% C.L.) or 425.6 +- 42.9 nb.
DOI: 10.17182/hepdata.64600.v1/t1
title: "Table 1" of "Measurement of the t-channel single-top-quark production cross section and of the |Vtb| CKM matrix element in pp collisions at sqrt(s) = 8 TeV"

description: The measured inclusive single-top-quark production cross section and the separate single top-quark and top-antiquark production cross sections in the t-channel.
description: CERN-LHC. Measurements are presented of the t-channel single-top-quark production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The results are based on a data sample corresponding to an integrated luminosity of 19.7 inverse femtobarns recorded with the CMS detector at the LHC during 2012. The cross section is measured inclusively, as well as separately for top quarks and antiquarks, in final states with a muon or an electron. The ratio of the inclusive production cross section measured using the 8 TeV dataset and a 7 TeV dataset, the ratio of the top quark and antiquark production cross sections and the modulus of the CKM matrix element V(TB) are also measured.
DOI: 10.17182/hepdata.64600.v1/t2
title: "Table 2" of "Measurement of the t-channel single-top-quark production cross section and of the |Vtb| CKM matrix element in pp collisions at sqrt(s) = 8 TeV"

description: The ratio of the inclusive single-top-quark production cross section in the t-channel at 8 TeV to the cross section at 7 TeV.
description: CERN-LHC. Measurements are presented of the t-channel single-top-quark production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The results are based on a data sample corresponding to an integrated luminosity of 19.7 inverse femtobarns recorded with the CMS detector at the LHC during 2012. The cross section is measured inclusively, as well as separately for top quarks and antiquarks, in final states with a muon or an electron. The ratio of the inclusive production cross section measured using the 8 TeV dataset and a 7 TeV dataset, the ratio of the top quark and antiquark production cross sections and the modulus of the CKM matrix element V(TB) are also measured.
DOI: 10.17182/hepdata.64600.v1/t3
title: "Table 3" of "Measurement of the t-channel single-top-quark production cross section and of the |Vtb| CKM matrix element in pp collisions at sqrt(s) = 8 TeV"

description: The ratio of the top-quark production cross section in the t-channel to the top-antiquark production cross section in the t-channel.
description: CERN-LHC. Measurements are presented of the t-channel single-top-quark production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The results are based on a data sample corresponding to an integrated luminosity of 19.7 inverse femtobarns recorded with the CMS detector at the LHC during 2012. The cross section is measured inclusively, as well as separately for top quarks and antiquarks, in final states with a muon or an electron. The ratio of the inclusive production cross section measured using the 8 TeV dataset and a 7 TeV dataset, the ratio of the top quark and antiquark production cross sections and the modulus of the CKM matrix element V(TB) are also measured.
DOI: 10.17182/hepdata.64600.v1/t4
title: "Table 4" of "Measurement of the t-channel single-top-quark production cross section and of the |Vtb| CKM matrix element in pp collisions at sqrt(s) = 8 TeV"

description: The modulus of the CKM matrix element V(TB), the first error comes from the uncertainties on the measurement of SIG(TOP TOPBAR) and the second error comes from the uncertainties on the theoretical value of SIG(TOP TOPBAR).
description: CERN-LHC. Measurements are presented of the t-channel single-top-quark production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The results are based on a data sample corresponding to an integrated luminosity of 19.7 inverse femtobarns recorded with the CMS detector at the LHC during 2012. The cross section is measured inclusively, as well as separately for top quarks and antiquarks, in final states with a muon or an electron. The ratio of the inclusive production cross section measured using the 8 TeV dataset and a 7 TeV dataset, the ratio of the top quark and antiquark production cross sections and the modulus of the CKM matrix element V(TB) are also measured.
DOI: 10.17182/hepdata.64605.v1/t1
title: "Table 1" of "Antideuteron production in $\Upsilon(nS)$ decays and in $e^+e^- \to q\overline{q}$ at $\sqrt{s} \approx 10.58 \mathrm{\,Ge\kern -0.1em V}$"

description: The rate of antideuteron production from the decay of UPSILON(3S).
description: SLAC-PEP2. We present measurements of the inclusive production of antideuterons in e+ e- annihilation into hadrons at approximately 10.58 GeV center-of-mass energy and in Upsilon(1S,2S,3S) decays. The results are obtained using data collected by the BABAR detector at the PEP-II electron-positron collider.
DOI: 10.17182/hepdata.64605.v1/t2
title: "Table 2" of "Antideuteron production in $\Upsilon(nS)$ decays and in $e^+e^- \to q\overline{q}$ at $\sqrt{s} \approx 10.58 \mathrm{\,Ge\kern -0.1em V}$"

description: The rate of antideuteron production from the decay of UPSILON(2S).
description: SLAC-PEP2. We present measurements of the inclusive production of antideuterons in e+ e- annihilation into hadrons at approximately 10.58 GeV center-of-mass energy and in Upsilon(1S,2S,3S) decays. The results are obtained using data collected by the BABAR detector at the PEP-II electron-positron collider.
DOI: 10.17182/hepdata.64605.v1/t3
title: "Table 3" of "Antideuteron production in $\Upsilon(nS)$ decays and in $e^+e^- \to q\overline{q}$ at $\sqrt{s} \approx 10.58 \mathrm{\,Ge\kern -0.1em V}$"

description: The rate of antideuteron production from the decay of UPSILON(1S).
description: SLAC-PEP2. We present measurements of the inclusive production of antideuterons in e+ e- annihilation into hadrons at approximately 10.58 GeV center-of-mass energy and in Upsilon(1S,2S,3S) decays. The results are obtained using data collected by the BABAR detector at the PEP-II electron-positron collider.
DOI: 10.17182/hepdata.64605.v1/t4
title: "Table 4" of "Antideuteron production in $\Upsilon(nS)$ decays and in $e^+e^- \to q\overline{q}$ at $\sqrt{s} \approx 10.58 \mathrm{\,Ge\kern -0.1em V}$"

description: The cross section of the process E+ E- --&gt; DEUTBAR X.
description: SLAC-PEP2. We present measurements of the inclusive production of antideuterons in e+ e- annihilation into hadrons at approximately 10.58 GeV center-of-mass energy and in Upsilon(1S,2S,3S) decays. The results are obtained using data collected by the BABAR detector at the PEP-II electron-positron collider.
DOI: 10.17182/hepdata.64605.v1/t5
title: "Table 5" of "Antideuteron production in $\Upsilon(nS)$ decays and in $e^+e^- \to q\overline{q}$ at $\sqrt{s} \approx 10.58 \mathrm{\,Ge\kern -0.1em V}$"

description: The ratio of the cross sections of the processes E+ E- --&gt; DEUTBAR X and E+ E- --&gt; HADRONS.
description: SLAC-PEP2. We present measurements of the inclusive production of antideuterons in e+ e- annihilation into hadrons at approximately 10.58 GeV center-of-mass energy and in Upsilon(1S,2S,3S) decays. The results are obtained using data collected by the BABAR detector at the PEP-II electron-positron collider.
DOI: 10.17182/hepdata.64611.v1/t1
title: "Table 1" of "Measurement of the 4l Cross Section at the Z Resonance and Determination of the Branching Fraction of Z-&gt;4l in pp Collisions at sqrt(s) = 7 and 8 TeV with ATLAS"

description: The measured individual cross sections in the fiducial region and the combined cross sections for 4-muon and 4-electron final states at a centre-of-collision energy of 7 TeV.
description: CERN-LHC. Measurements of four-lepton, where lepton refers to electrons and muons, production cross sections at the Z resonance in pp collisions at the LHC with the ATLAS detector are presented. The analysis uses data recorded in 2011 and 2012 and corresponds to an integrated luminosity of 4.5 fb^{-1} at 7 TeV and 20.3 fb^{-1} at 8 TeV.
DOI: 10.17182/hepdata.64611.v1/t2
title: "Table 2" of "Measurement of the 4l Cross Section at the Z Resonance and Determination of the Branching Fraction of Z-&gt;4l in pp Collisions at sqrt(s) = 7 and 8 TeV with ATLAS"

description: The measured individual cross sections in the fiducial region and the combined cross sections for 2-muon-2-electron final states at a centre-of-collision energy of 7 TeV.
description: CERN-LHC. Measurements of four-lepton, where lepton refers to electrons and muons, production cross sections at the Z resonance in pp collisions at the LHC with the ATLAS detector are presented. The analysis uses data recorded in 2011 and 2012 and corresponds to an integrated luminosity of 4.5 fb^{-1} at 7 TeV and 20.3 fb^{-1} at 8 TeV.
DOI: 10.17182/hepdata.64611.v1/t3
title: "Table 3" of "Measurement of the 4l Cross Section at the Z Resonance and Determination of the Branching Fraction of Z-&gt;4l in pp Collisions at sqrt(s) = 7 and 8 TeV with ATLAS"

description: The measured cross section for four-lepton final states at a centre-of-collision energy of 7 TeV.
description: CERN-LHC. Measurements of four-lepton, where lepton refers to electrons and muons, production cross sections at the Z resonance in pp collisions at the LHC with the ATLAS detector are presented. The analysis uses data recorded in 2011 and 2012 and corresponds to an integrated luminosity of 4.5 fb^{-1} at 7 TeV and 20.3 fb^{-1} at 8 TeV.
DOI: 10.17182/hepdata.64611.v1/t4
title: "Table 4" of "Measurement of the 4l Cross Section at the Z Resonance and Determination of the Branching Fraction of Z-&gt;4l in pp Collisions at sqrt(s) = 7 and 8 TeV with ATLAS"

description: The measured individual cross sections in the fiducial region and the combined cross sections for 4-muon and 4-electron final states at a centre-of-collision energy of 8 TeV.
description: CERN-LHC. Measurements of four-lepton, where lepton refers to electrons and muons, production cross sections at the Z resonance in pp collisions at the LHC with the ATLAS detector are presented. The analysis uses data recorded in 2011 and 2012 and corresponds to an integrated luminosity of 4.5 fb^{-1} at 7 TeV and 20.3 fb^{-1} at 8 TeV.
DOI: 10.17182/hepdata.64611.v1/t5
title: "Table 5" of "Measurement of the 4l Cross Section at the Z Resonance and Determination of the Branching Fraction of Z-&gt;4l in pp Collisions at sqrt(s) = 7 and 8 TeV with ATLAS"

description: The measured individual cross sections in the fiducial region and the combined cross sections for for 2-muon-2-electron final states at a centre-of-collision energy of 8 TeV.
description: CERN-LHC. Measurements of four-lepton, where lepton refers to electrons and muons, production cross sections at the Z resonance in pp collisions at the LHC with the ATLAS detector are presented. The analysis uses data recorded in 2011 and 2012 and corresponds to an integrated luminosity of 4.5 fb^{-1} at 7 TeV and 20.3 fb^{-1} at 8 TeV.
DOI: 10.17182/hepdata.64611.v1/t6
title: "Table 6" of "Measurement of the 4l Cross Section at the Z Resonance and Determination of the Branching Fraction of Z-&gt;4l in pp Collisions at sqrt(s) = 7 and 8 TeV with ATLAS"

description: The measured cross section for four-lepton final states at a centre-of-collision energy of 8 TeV.
description: CERN-LHC. Measurements of four-lepton, where lepton refers to electrons and muons, production cross sections at the Z resonance in pp collisions at the LHC with the ATLAS detector are presented. The analysis uses data recorded in 2011 and 2012 and corresponds to an integrated luminosity of 4.5 fb^{-1} at 7 TeV and 20.3 fb^{-1} at 8 TeV.
DOI: 10.17182/hepdata.64611.v1/t7
title: "Table 7" of "Measurement of the 4l Cross Section at the Z Resonance and Determination of the Branching Fraction of Z-&gt;4l in pp Collisions at sqrt(s) = 7 and 8 TeV with ATLAS"

description: The branching fraction for Z0 --&gt; 4 LEPTON, summed over all final states, measured using both the 7 and 8 TeV datasets.
description: CERN-LHC. Measurements of four-lepton, where lepton refers to electrons and muons, production cross sections at the Z resonance in pp collisions at the LHC with the ATLAS detector are presented. The analysis uses data recorded in 2011 and 2012 and corresponds to an integrated luminosity of 4.5 fb^{-1} at 7 TeV and 20.3 fb^{-1} at 8 TeV.
DOI: 10.17182/hepdata.64619.v1/t1
title: "Table 1" of "Measurement of WZ and ZZ production in pp collisions at sqrt(s) = 8 TeV in final states with b-tagged jets"

description: The cross section for inclusive WZ production for the mass range 60 &lt; M(Z) &lt; 120 GeV.
description: CERN-LHC. Measurements are reported of the WZ and ZZ production cross sections in proton-proton collisions at sqrt(s) = 8 TeV in final states where one Z boson decays to b-tagged jets. The other gauge boson, either W or Z, is detected through its leptonic decay (either W --&gt; E NUE, MU NUMU or Z0 --&gt; E+ E-, MU+ MU-, or NU NUBAR. The results are based on data corresponding to an integrated luminosity of 18.9 inverse-femtobarns collected with the CMS detector at the Large Hadron Collider.
DOI: 10.17182/hepdata.64619.v1/t2
title: "Table 2" of "Measurement of WZ and ZZ production in pp collisions at sqrt(s) = 8 TeV in final states with b-tagged jets"

description: The cross section for inclusive ZZ production for the mass range 60 &lt; M(Z) &lt; 120 GeV.
description: CERN-LHC. Measurements are reported of the WZ and ZZ production cross sections in proton-proton collisions at sqrt(s) = 8 TeV in final states where one Z boson decays to b-tagged jets. The other gauge boson, either W or Z, is detected through its leptonic decay (either W --&gt; E NUE, MU NUMU or Z0 --&gt; E+ E-, MU+ MU-, or NU NUBAR. The results are based on data corresponding to an integrated luminosity of 18.9 inverse-femtobarns collected with the CMS detector at the Large Hadron Collider.
DOI: 10.17182/hepdata.64619.v1/t3
title: "Table 3" of "Measurement of WZ and ZZ production in pp collisions at sqrt(s) = 8 TeV in final states with b-tagged jets"

description: The cross section for inclusive WZ production in the region defined by 60 &lt; M(Z) &lt; 120 GeV and PT(W) &gt; 100 GeV.
description: CERN-LHC. Measurements are reported of the WZ and ZZ production cross sections in proton-proton collisions at sqrt(s) = 8 TeV in final states where one Z boson decays to b-tagged jets. The other gauge boson, either W or Z, is detected through its leptonic decay (either W --&gt; E NUE, MU NUMU or Z0 --&gt; E+ E-, MU+ MU-, or NU NUBAR. The results are based on data corresponding to an integrated luminosity of 18.9 inverse-femtobarns collected with the CMS detector at the Large Hadron Collider.
DOI: 10.17182/hepdata.64619.v1/t4
title: "Table 4" of "Measurement of WZ and ZZ production in pp collisions at sqrt(s) = 8 TeV in final states with b-tagged jets"

description: The cross section for inclusive ZZ production in the region defined by 60 &lt; M(Z) &lt; 120 GeV and PT(Z(LEPTONIC)) &gt; 100 GeV.
description: CERN-LHC. Measurements are reported of the WZ and ZZ production cross sections in proton-proton collisions at sqrt(s) = 8 TeV in final states where one Z boson decays to b-tagged jets. The other gauge boson, either W or Z, is detected through its leptonic decay (either W --&gt; E NUE, MU NUMU or Z0 --&gt; E+ E-, MU+ MU-, or NU NUBAR. The results are based on data corresponding to an integrated luminosity of 18.9 inverse-femtobarns collected with the CMS detector at the Large Hadron Collider.
DOI: 10.17182/hepdata.64620.v1/t1
title: "Table 1" of "Search for Scalar Diphoton Resonances in the Mass Range $65-600$ GeV with the ATLAS Detector in $pp$ Collision Data at $\sqrt{s}$ = 8 $TeV$"

description: The measured fiducial cross section limit.
description: CERN-LHC-ATLAS. Measurement of the 95% CL limit on the fiducial production cross-section times branching ratio of a Higgs-like resonance decaying into two photons, as a function of the resonance mass mX. The resonance is assumed to be narrow. The narrow width assumption is valid for natural widths smaller than about 0.09 GeV + 0.01*mX. The interference of the resonance with the continuum background is neglected. The cross-section is reported for a fiducial volume defined as follows: photon |eta| &lt; 2.37, photon energies required to be E1 &gt; 22 GeV and E2 &gt; 22 GeV for mX &lt; 110 GeV. For mX &gt; 110 GeV, mass-dependent cuts are applied on top: E1/mgg &gt; 0.4 and E2/mgg &gt; 0.3, where mgg is the diphoton invariant mass. The particle-level isolation within a cone of size DR=0.4 around each photon is required to be less than 14 GeV.
DOI: 10.17182/hepdata.64626.v1/t1
title: "Table 1" of "Measurement of the ZZ Production Cross Section Using the Full CDF II Data Set"

description: The measured cross section for the process P PBAR --&gt; Z0 Z0 --&gt; LEPTON+ LEPTON- LEPTON+ LEPTON-.
description: Fermilab-Tevatron. We present a measurement of the ZZ boson-pair production cross section in 1.96 TeV center-of-mass energy ppbar collisions. We reconstruct final states incorporating four charged leptons or two charged leptons and two neutrinos from the full data set collected by the Collider Detector experiment during the period 2001 - 2011 at the Fermilab Tevatron, corresponding to 9.7 fb^{-1} of integrated luminosity.