cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.84818.v1/t22
title: "Table 22" of "Measurement of the four-lepton invariant mass spectrum in 13 TeV proton-proton collisions with the ATLAS detector"

description: Statistical covariance matrix for the differential $m_{4l}$-$y_{4l}$ distribution. <br><br> Bins labelled 1-9 correspond to the 0.0$&lt; y_{4l} &lt; $0.4 bin with $m_{4l}$ values as listed in Table 6.<br> Bins labelled 10-18 correspond to the 0.4$&lt; y_{4l} &lt;$0.8 bin with $m_{4l}$ values as listed in Table 7.<br> Bins labelled 19-26 correspond to the 0.8$&lt; y_{4l} &lt;$1.2 bin with $m_{4l}$ values as listed in Table 8.<br> Bins labelled 27-34 correspond to the 1.2$&lt; y_{4l} &lt;$2.5 bin with $m_{4l}$ values as listed in Table 9.
description: CERN-LHC. A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13 TeV delivered by the Large Hadron Collider. The differential cross section is measured for events containing two same-flavour opposite-sign lepton pairs, and is corrected for detector effects. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single Z production, Higgs production, and Z boson pair production, and non-negligible interference effects at high invariant masses. In addition, there may be contributions from beyond-the-Standard Model (BSM) physics. The measurement is compared to state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\to ZZ \to 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible BSM contribution.
DOI: 10.17182/hepdata.84818.v1/t23
title: "Table 23" of "Measurement of the four-lepton invariant mass spectrum in 13 TeV proton-proton collisions with the ATLAS detector"

description: Background covariance matrix for the differential $m_{4l}$-$y_{4l}$ distribution. <br><br> Bins labelled 1-9 correspond to the 0.0$&lt; y_{4l} &lt; $0.4 bin with $m_{4l}$ values as listed in Table 6.<br> Bins labelled 10-18 correspond to the 0.4$&lt; y_{4l} &lt;$0.8 bin with $m_{4l}$ values as listed in Table 7.<br> Bins labelled 19-26 correspond to the 0.8$&lt; y_{4l} &lt;$1.2 bin with $m_{4l}$ values as listed in Table 8.<br> Bins labelled 27-34 correspond to the 1.2$&lt; y_{4l} &lt;$2.5 bin with $m_{4l}$ values as listed in Table 9.
description: CERN-LHC. A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13 TeV delivered by the Large Hadron Collider. The differential cross section is measured for events containing two same-flavour opposite-sign lepton pairs, and is corrected for detector effects. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single Z production, Higgs production, and Z boson pair production, and non-negligible interference effects at high invariant masses. In addition, there may be contributions from beyond-the-Standard Model (BSM) physics. The measurement is compared to state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\to ZZ \to 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible BSM contribution.
DOI: 10.17182/hepdata.84818.v1/t24
title: "Table 24" of "Measurement of the four-lepton invariant mass spectrum in 13 TeV proton-proton collisions with the ATLAS detector"

description: Systematic covariance matrix for the differential $m_{4l}$-MELA distribution. <br><br> Bins labelled 1-7 correspond to the MELA$&lt;$ 0.4 bin with $m_{4l}$ values as listed in Table 10.<br> Bins labelled 8-12 correspond to the MELA$&gt;$ 0.4 bin with $m_{4l}$ values as listed in Table 11.
description: CERN-LHC. A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13 TeV delivered by the Large Hadron Collider. The differential cross section is measured for events containing two same-flavour opposite-sign lepton pairs, and is corrected for detector effects. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single Z production, Higgs production, and Z boson pair production, and non-negligible interference effects at high invariant masses. In addition, there may be contributions from beyond-the-Standard Model (BSM) physics. The measurement is compared to state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\to ZZ \to 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible BSM contribution.
DOI: 10.17182/hepdata.84818.v1/t25
title: "Table 25" of "Measurement of the four-lepton invariant mass spectrum in 13 TeV proton-proton collisions with the ATLAS detector"

description: Statistical covariance matrix for the differential $m_{4l}$-MELA distribution. <br><br> Bins labelled 1-7 correspond to the MELA$&lt;$ 0.4 bin with $m_{4l}$ values as listed in Table 10.<br> Bins labelled 8-12 correspond to the MELA$&gt;$ 0.4 bin with $m_{4l}$ values as listed in Table 11.
description: CERN-LHC. A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13 TeV delivered by the Large Hadron Collider. The differential cross section is measured for events containing two same-flavour opposite-sign lepton pairs, and is corrected for detector effects. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single Z production, Higgs production, and Z boson pair production, and non-negligible interference effects at high invariant masses. In addition, there may be contributions from beyond-the-Standard Model (BSM) physics. The measurement is compared to state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\to ZZ \to 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible BSM contribution.
DOI: 10.17182/hepdata.84818.v1/t26
title: "Table 26" of "Measurement of the four-lepton invariant mass spectrum in 13 TeV proton-proton collisions with the ATLAS detector"

description: Background covariance matrix for the differential $m_{4l}$-MELA distribution. <br><br> Bins labelled 1-7 correspond to the MELA$&lt;$ 0.4 bin with $m_{4l}$ values as listed in Table 10.<br> Bins labelled 8-12 correspond to the MELA$&gt;$ 0.4 bin with $m_{4l}$ values as listed in Table 11.
description: CERN-LHC. A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13 TeV delivered by the Large Hadron Collider. The differential cross section is measured for events containing two same-flavour opposite-sign lepton pairs, and is corrected for detector effects. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single Z production, Higgs production, and Z boson pair production, and non-negligible interference effects at high invariant masses. In addition, there may be contributions from beyond-the-Standard Model (BSM) physics. The measurement is compared to state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\to ZZ \to 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible BSM contribution.
DOI: 10.17182/hepdata.84818.v1/t27
title: "Table 27" of "Measurement of the four-lepton invariant mass spectrum in 13 TeV proton-proton collisions with the ATLAS detector"

description: Systematic covariance matrix for the differential $m_{4l}$-lepton flavour distribution. <br><br> Bins labelled 1-9 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 12.<br> Bins labelled 10-18 correspond to $eeee$ events with $m_{4l}$ values as listed in Table 13.<br> Bins labelled 19-27 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 14.<br>
description: CERN-LHC. A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13 TeV delivered by the Large Hadron Collider. The differential cross section is measured for events containing two same-flavour opposite-sign lepton pairs, and is corrected for detector effects. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single Z production, Higgs production, and Z boson pair production, and non-negligible interference effects at high invariant masses. In addition, there may be contributions from beyond-the-Standard Model (BSM) physics. The measurement is compared to state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\to ZZ \to 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible BSM contribution.
DOI: 10.17182/hepdata.84818.v1/t28
title: "Table 28" of "Measurement of the four-lepton invariant mass spectrum in 13 TeV proton-proton collisions with the ATLAS detector"

description: Statistical covariance matrix for the differential $m_{4l}$-lepton flavour distribution. <br><br> Bins labelled 1-9 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 12.<br> Bins labelled 10-18 correspond to $eeee$ events with $m_{4l}$ values as listed in Table 13.<br> Bins labelled 19-27 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 14.<br>
description: CERN-LHC. A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13 TeV delivered by the Large Hadron Collider. The differential cross section is measured for events containing two same-flavour opposite-sign lepton pairs, and is corrected for detector effects. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single Z production, Higgs production, and Z boson pair production, and non-negligible interference effects at high invariant masses. In addition, there may be contributions from beyond-the-Standard Model (BSM) physics. The measurement is compared to state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\to ZZ \to 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible BSM contribution.
DOI: 10.17182/hepdata.84818.v1/t29
title: "Table 29" of "Measurement of the four-lepton invariant mass spectrum in 13 TeV proton-proton collisions with the ATLAS detector"

description: Background covariance matrix for the differential $m_{4l}$-lepton flavour distribution. <br><br> Bins labelled 1-9 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 12.<br> Bins labelled 10-18 correspond to $eeee$ events with $m_{4l}$ values as listed in Table 13.<br> Bins labelled 19-27 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 14.<br>
description: CERN-LHC. A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13 TeV delivered by the Large Hadron Collider. The differential cross section is measured for events containing two same-flavour opposite-sign lepton pairs, and is corrected for detector effects. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single Z production, Higgs production, and Z boson pair production, and non-negligible interference effects at high invariant masses. In addition, there may be contributions from beyond-the-Standard Model (BSM) physics. The measurement is compared to state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\to ZZ \to 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible BSM contribution.
DOI: 10.25549/stayathome-c125-44
title: #StayAtHome 2020

description: How does COVID-19 impact the University of Southern California community?USC Libraries makes an effort to collect and archive materials and stories from individuals from the University of Southern California, Los Angeles, and the Southern California community as a way to create a public record of the coronavirus COVID-19 pandemic that will be used for research and other purposes.Submissions will be archived and processed by USC Libraries Special Collections and USC.Libraries Digital Library. Submissions will only be viewed by the #StayAtHome project team. If you have any questions or comments please visit our website. We have an FAQ, helpful submission guidelines, and project team information with direct contact details: https://libguides.usc.edu/stayathome.There is a companion Website (https://stayathomeusc.github.io/stayathome/) to USC's #StayAtHome archiving project. The map will provide access to a selection of contributions which you can select and read more about.
DOI: 10.25549/stayathome-c125-15
title: #StayAtHome 2020

description: How does COVID-19 impact the University of Southern California community?USC Libraries makes an effort to collect and archive materials and stories from individuals from the University of Southern California, Los Angeles, and the Southern California community as a way to create a public record of the coronavirus COVID-19 pandemic that will be used for research and other purposes.Submissions will be archived and processed by USC Libraries Special Collections and USC.Libraries Digital Library. Submissions will only be viewed by the #StayAtHome project team. If you have any questions or comments please visit our website. We have an FAQ, helpful submission guidelines, and project team information with direct contact details: https://libguides.usc.edu/stayathome.There is a companion Website (https://stayathomeusc.github.io/stayathome/) to USC's #StayAtHome archiving project. The map will provide access to a selection of contributions which you can select and read more about.
DOI: 10.17182/hepdata.84820.v1/t1
title: "Table 1" of "Cross-section measurements of the Higgs boson decaying to a pair of tau leptons in proton--proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: “Yields in the leplep boost loose category“
description: A measurement of total production cross sections of the Higgs boson in proton-proton collisions is presented in the H -&gt; tau tau decay channel. The analysis is performed using 36.1 fb-1 of data recorded by the ATLAS experiment at the Large Hadron Collider at a center-of-mass energy of 13 TeV. All combinations of leptonic and hadronic tau decays are considered. The H-&gt;tau tau signal over the expected background from other Standard Model processes is established with an observed (expected) significance of 4.4 (4.1) standard deviations. Combined with results using data taken at 7 and 8 TeV centre-of-mass energies, the observed (expected) significance amounts to 6.4 (5.4) standard deviations and constitutes an observation of H-&gt;tautau decays by the ATLAS experiment. . 

 Object definition: 
- Electron candidates are required to pass the loose likelihood-based identification selection, to have transverse momentum PT &gt; 15 GeV and |eta| &lt; 2.47, excluding the region 1.37&lt; | eta | &lt; 1.52. 
 - The muon candidates are required to have PT &gt; 10 GeV and |eta| &lt;2.5 and to pass the loose muon identification requirements. 
 - The tau candidates are required to have PT &gt; 20 GeV, to have one or three associated tracks and an absolute electric charge of one. They have to pass the loose identification requirement 
 - Jets are reconstructed from topological clusters in the calorimeter using the anti-Kt algorithm with a radius parameter value R = 0.4. 

 Signal region definition: 
- VBF region: this region is characterized by the presence of two jets with PT &gt; 40 GeV and PT &gt; 30GeV, respectively.In addition, the two jets are required to be in opposite hemispheres of the detector with a large pseudorapidity separation of |Delta eta (jet,jet)| &gt; 3 and their invariant mass, M(jet,jet) is required to be larger than 400 GeV. The selected leptons are required to have eta values that lie between those of the two jets. 
 - ggH region: It contains all events with PTH &gt; 100 GeV that do not pass the VBF selection 

 Using PTH, Delta R(tau,tau) and M(jet,jet), both inclusive categories are split further into 13 exclusive signal regions with different signal-to-background ratios to improve the sensitivity

 The cross sections for the ggH and VBFH processes have been also measured according to the definitions of the STXS framework in the following bins: 
 - ggH Low Boost: N jets &gt; 0, 60 GeV &lt; PTH &lt; 120 GeV, |eta(H)| &lt; 2.5 
 - ggH High Boost: N jets &gt; 0, PTH &gt; 120 GeV, |eta(H)| &lt; 2.5 
 - VBF : |eta(H)| &lt; 2.5
DOI: 10.17182/hepdata.84820.v1/t2
title: "Table 2" of "Cross-section measurements of the Higgs boson decaying to a pair of tau leptons in proton--proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: “Yields in the leplep boost tight category“
description: A measurement of total production cross sections of the Higgs boson in proton-proton collisions is presented in the H -&gt; tau tau decay channel. The analysis is performed using 36.1 fb-1 of data recorded by the ATLAS experiment at the Large Hadron Collider at a center-of-mass energy of 13 TeV. All combinations of leptonic and hadronic tau decays are considered. The H-&gt;tau tau signal over the expected background from other Standard Model processes is established with an observed (expected) significance of 4.4 (4.1) standard deviations. Combined with results using data taken at 7 and 8 TeV centre-of-mass energies, the observed (expected) significance amounts to 6.4 (5.4) standard deviations and constitutes an observation of H-&gt;tautau decays by the ATLAS experiment. . 

 Object definition: 
- Electron candidates are required to pass the loose likelihood-based identification selection, to have transverse momentum PT &gt; 15 GeV and |eta| &lt; 2.47, excluding the region 1.37&lt; | eta | &lt; 1.52. 
 - The muon candidates are required to have PT &gt; 10 GeV and |eta| &lt;2.5 and to pass the loose muon identification requirements. 
 - The tau candidates are required to have PT &gt; 20 GeV, to have one or three associated tracks and an absolute electric charge of one. They have to pass the loose identification requirement 
 - Jets are reconstructed from topological clusters in the calorimeter using the anti-Kt algorithm with a radius parameter value R = 0.4. 

 Signal region definition: 
- VBF region: this region is characterized by the presence of two jets with PT &gt; 40 GeV and PT &gt; 30GeV, respectively.In addition, the two jets are required to be in opposite hemispheres of the detector with a large pseudorapidity separation of |Delta eta (jet,jet)| &gt; 3 and their invariant mass, M(jet,jet) is required to be larger than 400 GeV. The selected leptons are required to have eta values that lie between those of the two jets. 
 - ggH region: It contains all events with PTH &gt; 100 GeV that do not pass the VBF selection 

 Using PTH, Delta R(tau,tau) and M(jet,jet), both inclusive categories are split further into 13 exclusive signal regions with different signal-to-background ratios to improve the sensitivity

 The cross sections for the ggH and VBFH processes have been also measured according to the definitions of the STXS framework in the following bins: 
 - ggH Low Boost: N jets &gt; 0, 60 GeV &lt; PTH &lt; 120 GeV, |eta(H)| &lt; 2.5 
 - ggH High Boost: N jets &gt; 0, PTH &gt; 120 GeV, |eta(H)| &lt; 2.5 
 - VBF : |eta(H)| &lt; 2.5
DOI: 10.17182/hepdata.84820.v1/t3
title: "Table 3" of "Cross-section measurements of the Higgs boson decaying to a pair of tau leptons in proton--proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: “Yields in the leplep boost top control region“
description: A measurement of total production cross sections of the Higgs boson in proton-proton collisions is presented in the H -&gt; tau tau decay channel. The analysis is performed using 36.1 fb-1 of data recorded by the ATLAS experiment at the Large Hadron Collider at a center-of-mass energy of 13 TeV. All combinations of leptonic and hadronic tau decays are considered. The H-&gt;tau tau signal over the expected background from other Standard Model processes is established with an observed (expected) significance of 4.4 (4.1) standard deviations. Combined with results using data taken at 7 and 8 TeV centre-of-mass energies, the observed (expected) significance amounts to 6.4 (5.4) standard deviations and constitutes an observation of H-&gt;tautau decays by the ATLAS experiment. . 

 Object definition: 
- Electron candidates are required to pass the loose likelihood-based identification selection, to have transverse momentum PT &gt; 15 GeV and |eta| &lt; 2.47, excluding the region 1.37&lt; | eta | &lt; 1.52. 
 - The muon candidates are required to have PT &gt; 10 GeV and |eta| &lt;2.5 and to pass the loose muon identification requirements. 
 - The tau candidates are required to have PT &gt; 20 GeV, to have one or three associated tracks and an absolute electric charge of one. They have to pass the loose identification requirement 
 - Jets are reconstructed from topological clusters in the calorimeter using the anti-Kt algorithm with a radius parameter value R = 0.4. 

 Signal region definition: 
- VBF region: this region is characterized by the presence of two jets with PT &gt; 40 GeV and PT &gt; 30GeV, respectively.In addition, the two jets are required to be in opposite hemispheres of the detector with a large pseudorapidity separation of |Delta eta (jet,jet)| &gt; 3 and their invariant mass, M(jet,jet) is required to be larger than 400 GeV. The selected leptons are required to have eta values that lie between those of the two jets. 
 - ggH region: It contains all events with PTH &gt; 100 GeV that do not pass the VBF selection 

 Using PTH, Delta R(tau,tau) and M(jet,jet), both inclusive categories are split further into 13 exclusive signal regions with different signal-to-background ratios to improve the sensitivity

 The cross sections for the ggH and VBFH processes have been also measured according to the definitions of the STXS framework in the following bins: 
 - ggH Low Boost: N jets &gt; 0, 60 GeV &lt; PTH &lt; 120 GeV, |eta(H)| &lt; 2.5 
 - ggH High Boost: N jets &gt; 0, PTH &gt; 120 GeV, |eta(H)| &lt; 2.5 
 - VBF : |eta(H)| &lt; 2.5