cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.78377.v1/t18
title: "Exclusion contour 2 (exp.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Expected exclusion contours in chargino chargino and chargino neutralino production model.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t19
title: "X-section U.L. 1" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Observed upper limits on the model cross-section in units of pb as a function of the chargino and neutralino masses in chargino chargino pair production.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t20
title: "X-section U.L. 2" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Observed upper limits on the model cross-section in units of pb as a function of the chargino and neutralino masses in chargino chargino and chargino neutralino pair production.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t21
title: "Best SR" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Best signal region used in chargino chargino and chargino neutralino pair production, H is corresponding to SR-highMass and L is SR-lowMass.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t22
title: "1D limit 1 (obs.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Observed CLs significance in variable-x model of chargino chargino pair production for compressed mass scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t23
title: "1D limit 1 (exp.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Expected CLs significance in variable-x model of chargino chargino pair production for compressed mass scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t24
title: "1D limit 2 (obs.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Observed CLs significance in variable-x model of chargino chargino pair production for large mass splitting scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t25
title: "1D limit 2 (exp.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Expected CLs significance in variable-x model of chargino chargino pair production for large mass splitting scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t26
title: "1D limit 3 (obs.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Observed CLs significance in variable-x model of chargino chargino and chargino neutralino pair production for compressed mass scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t27
title: "1D limit 3 (exp.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Expected CLs significance in variable-x model of chargino chargino and chargino neutralino pair production for compressed mass scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t28
title: "1D limit 4 (obs.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Observed CLs significance in variable-x model of chargino chargino and chargino neutralino pair production for large mass splitting scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t29
title: "1D limit 4 (exp.)" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Expected CLs significance in variable-x model of chargino chargino and chargino neutralino pair production for large mass splitting scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t30
title: "Acceptance 1" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Acceptance in SR-lowMass for CHARGINO1 NEUTRALINO2 production.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t31
title: "Acceptance 2" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Acceptance in SR-highMass for CHARGINO1 NEUTRALINO2 production.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t32
title: "Acceptance 3" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Acceptance in SR-highMass for CHARGINO1 CHARGINO1 production.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t33
title: "Efficiency 1" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Efficiency in SR-lowMass for CHARGINO1 NEUTRALINO2 production.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t34
title: "Efficiency 2" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Efficiency in SR-highMass for CHARGINO1 NEUTRALINO2 production.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t35
title: "Efficiency 3" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Efficiency in SR-highMass for CHARGINO1 CHARGINO1 production.
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t36
title: "Cutflow 1" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Cut flow for the reference point 1 (CHARGINO1 NEUTRALINO2 production) in SR-lowMass. The column labelled $N_{raw}$ shows the results for the generated number of events, while $N_{weighted}$ includes all correction factors applied to simulation, and is normalised to 36.1 fb$^{-1}$. The quoted uncertainties are statistical only. At the step ``at least two medium tau candidates, matched to trigger objects' the following requirements are applied: the event is recorded using either the asymmetric di-tau trigger or the di-tau+$E_{\mathrm T}^{\mathrm{miss}}$ trigger, and the two matched tau candidates must be of medium quality. If the event has been selected by the asymmetric di-tau trigger, the two tau candidates are required to have ${p}_{\mathrm{T}, \tau_1}&gt;$ 95 GeV and ${p}_{\mathrm{T}, \tau_2}&gt;$ 65 GeV. If the event has been selected by the di-tau+$E_{\mathrm T}^{\mathrm{miss}}$ trigger, the two tau candidates are required to have ${p}_{\mathrm{T}, \tau_1}&gt;$ 50 GeV, ${p}_{\mathrm{T}, \tau_2}&gt;$ 40 GeV, and $E_{\mathrm T}^{\mathrm{miss}}$ &gt; 150 GeV is required.}
description: No data abstract available.
DOI: 10.17182/hepdata.78377.v1/t37
title: "Cutflow 2" of "Search for the direct production of charginos and neutralinos in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector"

description: Cut flow for the reference point 2 (CHARGINO1 CHARGINO1 production) in SR-highMass. The column labelled $N_{raw}$ shows the results for the generated number of events, while $N_{weighted}$ includes all correction factors applied to simulation, and is normalised to 36.1 fb$^{-1}$. The quoted uncertainties are statistical only. At the step ``at least two medium tau candidates, matched to trigger objects' the following requirements are applied: the event is recorded using either the asymmetric di-tau trigger or the di-tau+$E_{\mathrm T}^{\mathrm{miss}}$ trigger, and the two matched tau candidates must be of medium quality. If the event has been selected by the asymmetric di-tau trigger, the two tau candidates are required to have ${p}_{\mathrm{T}, \tau_1}&gt;$ 95 GeV and ${p}_{\mathrm{T}, \tau_2}&gt;$ 65 GeV. If the event has been selected by the di-tau+$E_{\mathrm T}^{\mathrm{miss}}$ trigger, the two tau candidates are required to have ${p}_{\mathrm{T}, \tau_1}&gt;$ 50 GeV, ${p}_{\mathrm{T}, \tau_2}&gt;$ 40 GeV, and $E_{\mathrm T}^{\mathrm{miss}}$ &gt; 150 GeV is required.}
description: No data abstract available.
DOI: 10.17182/hepdata.78379.v1/t1
title: "Table 3" of "Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Measurement of signal strength
description: No data abstract available.
DOI: 10.17182/hepdata.78379.v1/t2
title: "Table 1" of "Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Event yields for the expected signal (S) and background (B) processes, and numbers of the observed data events in different categories. The full widths at half maximum (FWHM) of the signal $m_{μμ}$ distributions are also shown. In each category, the event yields are counted within an $m_{μμ}$ interval, which is centered at the simulated signal peak and contains 90% of the expected signal events. The expected signal event yields are normalized to $36.1 fb^-1$. The background in each category is normalized to the observed data yield, while the relative fractions between the different processes are fixed to the SM predictions.
description: No data abstract available.
DOI: 10.17182/hepdata.78379.v1/t3
title: "Table 2" of "Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The 95% CL upper limit on signal strength
description: No data abstract available.
DOI: 10.15468/dl.j7xvbc
title: Occurrence Download

description: A dataset containing 648 species occurrences available in GBIF matching the query:
{
 "DatasetKey" : [
 "is Rocky Mountain Biological Laboratory Mammal Collection"
 ]
}

 The dataset includes 648 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015415-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.78399.v1/t1
title: "Table 1" of "Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings"

description: Measured fiducial cross section in the WV-&gt;lvjj and WV-&gt;lvJ channels. Refer to the paper for details of applied event selection.
description: CERN-LHC. This paper presents a study of the production of WW or WZ boson pairs, with one W boson decaying to electron-neutrino or muon-neutrino and one W or Z boson decaying hadronically. The analysis uses 20.2 fb-1 of sqrt(s)=8 TeV pp collision data, collected by the ATLAS detector at the Large Hadron Collider. Cross-sections for WW/WZ production are measured in high-pT fiducial regions defined close to the experimental event selection. The cross-section is measured for the case where the hadronically decaying boson is reconstructed as two resolved jets (WV-&gt;lvjj), and the case where it is reconstructed as a single jet (WV-&gt;lvJ). For the description of the WV-&gt;lvjj and WV-&gt;lvJ fiducial phase spaces, refer to section 8.1 and 8.2 of the paper.
The transverse momentum distribution of the hadronically decaying boson is used to search for new physics. Observations are consistent with the Standard Model predictions, and 95% confidence intervals are calculated for parameters describing anomalous triple gauge-boson couplings (aTGCs). The aTGC search is done applying the same selection used for cross section measurement, plus an additional requirement for the jet-jet invariant mass (single jet mass) to be close to the W mass: 65 GeV &lt; m_jj &lt; 95 GeV (65 GeV &lt; m_J &lt; 95 GeV).
DOI: 10.17182/hepdata.78399.v1/t2
title: "Table 2" of "Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings"

description: Correction factors D for WV-&gt;lvjj and WV-&gt;lvJ channels. D = fWW * CWW + (1-fWW) * CWZ. fWW is the predicted ratio of the WW fiducial cross section to the WW+WZ fiducial cross section: fWW = SIG_theo_WW * AWW / (SIG_theo_WW*AWW + SIG_theo_WZ*AWZ).
description: CERN-LHC. This paper presents a study of the production of WW or WZ boson pairs, with one W boson decaying to electron-neutrino or muon-neutrino and one W or Z boson decaying hadronically. The analysis uses 20.2 fb-1 of sqrt(s)=8 TeV pp collision data, collected by the ATLAS detector at the Large Hadron Collider. Cross-sections for WW/WZ production are measured in high-pT fiducial regions defined close to the experimental event selection. The cross-section is measured for the case where the hadronically decaying boson is reconstructed as two resolved jets (WV-&gt;lvjj), and the case where it is reconstructed as a single jet (WV-&gt;lvJ). For the description of the WV-&gt;lvjj and WV-&gt;lvJ fiducial phase spaces, refer to section 8.1 and 8.2 of the paper.
The transverse momentum distribution of the hadronically decaying boson is used to search for new physics. Observations are consistent with the Standard Model predictions, and 95% confidence intervals are calculated for parameters describing anomalous triple gauge-boson couplings (aTGCs). The aTGC search is done applying the same selection used for cross section measurement, plus an additional requirement for the jet-jet invariant mass (single jet mass) to be close to the W mass: 65 GeV &lt; m_jj &lt; 95 GeV (65 GeV &lt; m_J &lt; 95 GeV).
DOI: 10.17182/hepdata.78399.v1/t3
title: "Table 3" of "Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings"

description: The expected and observed 95% confidence intervals for the anomalous coupling parameters defined in the EFT frame work. WV-&gt;lvjj channel.
description: CERN-LHC. This paper presents a study of the production of WW or WZ boson pairs, with one W boson decaying to electron-neutrino or muon-neutrino and one W or Z boson decaying hadronically. The analysis uses 20.2 fb-1 of sqrt(s)=8 TeV pp collision data, collected by the ATLAS detector at the Large Hadron Collider. Cross-sections for WW/WZ production are measured in high-pT fiducial regions defined close to the experimental event selection. The cross-section is measured for the case where the hadronically decaying boson is reconstructed as two resolved jets (WV-&gt;lvjj), and the case where it is reconstructed as a single jet (WV-&gt;lvJ). For the description of the WV-&gt;lvjj and WV-&gt;lvJ fiducial phase spaces, refer to section 8.1 and 8.2 of the paper.
The transverse momentum distribution of the hadronically decaying boson is used to search for new physics. Observations are consistent with the Standard Model predictions, and 95% confidence intervals are calculated for parameters describing anomalous triple gauge-boson couplings (aTGCs). The aTGC search is done applying the same selection used for cross section measurement, plus an additional requirement for the jet-jet invariant mass (single jet mass) to be close to the W mass: 65 GeV &lt; m_jj &lt; 95 GeV (65 GeV &lt; m_J &lt; 95 GeV).
DOI: 10.17182/hepdata.78399.v1/t4
title: "Table 4" of "Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings"

description: The expected and observed 95% confidence intervals for the anomalous coupling parameters defined in the EFT frame work. WV-&gt;lvJ channel.
description: CERN-LHC. This paper presents a study of the production of WW or WZ boson pairs, with one W boson decaying to electron-neutrino or muon-neutrino and one W or Z boson decaying hadronically. The analysis uses 20.2 fb-1 of sqrt(s)=8 TeV pp collision data, collected by the ATLAS detector at the Large Hadron Collider. Cross-sections for WW/WZ production are measured in high-pT fiducial regions defined close to the experimental event selection. The cross-section is measured for the case where the hadronically decaying boson is reconstructed as two resolved jets (WV-&gt;lvjj), and the case where it is reconstructed as a single jet (WV-&gt;lvJ). For the description of the WV-&gt;lvjj and WV-&gt;lvJ fiducial phase spaces, refer to section 8.1 and 8.2 of the paper.
The transverse momentum distribution of the hadronically decaying boson is used to search for new physics. Observations are consistent with the Standard Model predictions, and 95% confidence intervals are calculated for parameters describing anomalous triple gauge-boson couplings (aTGCs). The aTGC search is done applying the same selection used for cross section measurement, plus an additional requirement for the jet-jet invariant mass (single jet mass) to be close to the W mass: 65 GeV &lt; m_jj &lt; 95 GeV (65 GeV &lt; m_J &lt; 95 GeV).
DOI: 10.17182/hepdata.78399.v1/t5
title: "Table 5" of "Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings"

description: The expected number of events passing the final event selection in the WW/WZ-&gt;lvjj channel, in each pT(jj) bin of the signal region (SR). The expected number of background and signal events are given, together with the number of events observed in data. The numbers correspond to Figures 7(a). The BSM numbers do not include the SM WV contribution, so the SM and BSM WV numbers should be added together. The numbers correspond to the raw event yields, not divided by the bin widths. The six bins in the SR have the following bin boundaries: (100, 200, 300, 400, 600, 800, +inf) GeV.
description: CERN-LHC. This paper presents a study of the production of WW or WZ boson pairs, with one W boson decaying to electron-neutrino or muon-neutrino and one W or Z boson decaying hadronically. The analysis uses 20.2 fb-1 of sqrt(s)=8 TeV pp collision data, collected by the ATLAS detector at the Large Hadron Collider. Cross-sections for WW/WZ production are measured in high-pT fiducial regions defined close to the experimental event selection. The cross-section is measured for the case where the hadronically decaying boson is reconstructed as two resolved jets (WV-&gt;lvjj), and the case where it is reconstructed as a single jet (WV-&gt;lvJ). For the description of the WV-&gt;lvjj and WV-&gt;lvJ fiducial phase spaces, refer to section 8.1 and 8.2 of the paper.
The transverse momentum distribution of the hadronically decaying boson is used to search for new physics. Observations are consistent with the Standard Model predictions, and 95% confidence intervals are calculated for parameters describing anomalous triple gauge-boson couplings (aTGCs). The aTGC search is done applying the same selection used for cross section measurement, plus an additional requirement for the jet-jet invariant mass (single jet mass) to be close to the W mass: 65 GeV &lt; m_jj &lt; 95 GeV (65 GeV &lt; m_J &lt; 95 GeV).
DOI: 10.17182/hepdata.78399.v1/t6
title: "Table 6" of "Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings"

description: The expected number of events passing the final event selection in the WW/WZ-&gt;lvjj channel, in each pT(jj) bin of the sideband control region (CR). The expected number of background and signal events are given, together with the number of events observed in data. The numbers correspond to Figures 6 of auxiliary material. The BSM numbers do not include the SM WV contribution, so the SM and BSM WV numbers should be added together. The numbers correspond to the raw event yields, not divided by the bin widths. The four bins in the CR have the following bin boundaries: (100, 200, 300, 700, +inf) GeV.
description: CERN-LHC. This paper presents a study of the production of WW or WZ boson pairs, with one W boson decaying to electron-neutrino or muon-neutrino and one W or Z boson decaying hadronically. The analysis uses 20.2 fb-1 of sqrt(s)=8 TeV pp collision data, collected by the ATLAS detector at the Large Hadron Collider. Cross-sections for WW/WZ production are measured in high-pT fiducial regions defined close to the experimental event selection. The cross-section is measured for the case where the hadronically decaying boson is reconstructed as two resolved jets (WV-&gt;lvjj), and the case where it is reconstructed as a single jet (WV-&gt;lvJ). For the description of the WV-&gt;lvjj and WV-&gt;lvJ fiducial phase spaces, refer to section 8.1 and 8.2 of the paper.
The transverse momentum distribution of the hadronically decaying boson is used to search for new physics. Observations are consistent with the Standard Model predictions, and 95% confidence intervals are calculated for parameters describing anomalous triple gauge-boson couplings (aTGCs). The aTGC search is done applying the same selection used for cross section measurement, plus an additional requirement for the jet-jet invariant mass (single jet mass) to be close to the W mass: 65 GeV &lt; m_jj &lt; 95 GeV (65 GeV &lt; m_J &lt; 95 GeV).