cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.84820.v1/t20
title: "Table 20" 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: “95% confidence level on ggH Vs VBFH cross section“
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/t21
title: "Table 21" 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: “68% confidence level on ggH Vs VBFH cross section“
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/t22
title: "Table 22" 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: “Observed and SM expected ggH and VBFH cross sections“
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/t23
title: "Table 23" 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: “Observed and SM expected total cross section per decay channel“
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/t24
title: "Table 24" 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: “Observed and SM expected total cross section per 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/t25
title: "Table 25" 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: “Observed and SM expected ggH and VBFH cross sections in exclusive regions of phase space of particle-level events“
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.84821.v1/t1
title: "Figure 1A : 60-80% Au+Au collisions" of "Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\sqrt{s_{NN}}$ = 193 GeV at STAR"

description: The centrality dependence of e+e− invariant mass spectra within the STAR acceptance from Au+Au collisions and U+U collisions for pair pT &lt; 0.15 GeV/c. The vertical bars on data points depict the statistical uncertainties, while the systematic uncertainties are shown as gray boxes. The hadronic cocktail yields from U+U collisions are ∼5%–12% higher than those from Au+Au collisions in given centrality bins; thus only cocktails for Au+Au collisions are shown here as solid lines, with shaded bands representing the systematic uncertainties for clarity.
description: Low-pT e+e− pair production in Au+Au collisions at $\sqrt{s_{{NN}}}$ = 200 GeV and U+U collisions at $\sqrt{s_{{NN}}}$ = 193 GeV at STAR
DOI: 10.17182/hepdata.84821.v1/t2
title: "Figure 1A : 60-80% U+U collisions" of "Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\sqrt{s_{NN}}$ = 193 GeV at STAR"

description: The centrality dependence of e+e− invariant mass spectra within the STAR acceptance from Au+Au collisions and U+U collisions for pair pT &lt; 0.15 GeV/c. The vertical bars on data points depict the statistical uncertainties, while the systematic uncertainties are shown as gray boxes. The hadronic cocktail yields from U+U collisions are ∼5%–12% higher than those from Au+Au collisions in given centrality bins; thus only cocktails for Au+Au collisions are shown here as solid lines, with shaded bands representing the systematic uncertainties for clarity.
description: Low-pT e+e− pair production in Au+Au collisions at $\sqrt{s_{{NN}}}$ = 200 GeV and U+U collisions at $\sqrt{s_{{NN}}}$ = 193 GeV at STAR
DOI: 10.17182/hepdata.84821.v1/t4
title: "Figure 1A : 40-60% U+U collisions" of "Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\sqrt{s_{NN}}$ = 193 GeV at STAR"

description: The centrality dependence of e+e− invariant mass spectra within the STAR acceptance from Au+Au collisions and U+U collisions for pair pT &lt; 0.15 GeV/c. The vertical bars on data points depict the statistical uncertainties, while the systematic uncertainties are shown as gray boxes. The hadronic cocktail yields from U+U collisions are ∼5%–12% higher than those from Au+Au collisions in given centrality bins; thus only cocktails for Au+Au collisions are shown here as solid lines, with shaded bands representing the systematic uncertainties for clarity.
description: Low-pT e+e− pair production in Au+Au collisions at $\sqrt{s_{{NN}}}$ = 200 GeV and U+U collisions at $\sqrt{s_{{NN}}}$ = 193 GeV at STAR
DOI: 10.25549/stayathome-c125-13
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.84821.v1/t3
title: "Figure 1A : 40-60% Au+Au collisions" of "Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\sqrt{s_{NN}}$ = 193 GeV at STAR"

description: The centrality dependence of e+e− invariant mass spectra within the STAR acceptance from Au+Au collisions and U+U collisions for pair pT &lt; 0.15 GeV/c. The vertical bars on data points depict the statistical uncertainties, while the systematic uncertainties are shown as gray boxes. The hadronic cocktail yields from U+U collisions are ∼5%–12% higher than those from Au+Au collisions in given centrality bins; thus only cocktails for Au+Au collisions are shown here as solid lines, with shaded bands representing the systematic uncertainties for clarity.
description: Low-pT e+e− pair production in Au+Au collisions at $\sqrt{s_{{NN}}}$ = 200 GeV and U+U collisions at $\sqrt{s_{{NN}}}$ = 193 GeV at STAR
DOI: 10.17182/hepdata.84821.v1/t5
title: "Figure 1A : 10-40% Au+Au collisions" of "Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\sqrt{s_{NN}}$ = 193 GeV at STAR"

description: The centrality dependence of e+e− invariant mass spectra within the STAR acceptance from Au+Au collisions and U+U collisions for pair pT &lt; 0.15 GeV/c. The vertical bars on data points depict the statistical uncertainties, while the systematic uncertainties are shown as gray boxes. The hadronic cocktail yields from U+U collisions are ∼5%–12% higher than those from Au+Au collisions in given centrality bins; thus only cocktails for Au+Au collisions are shown here as solid lines, with shaded bands representing the systematic uncertainties for clarity.
description: Low-pT e+e− pair production in Au+Au collisions at $\sqrt{s_{{NN}}}$ = 200 GeV and U+U collisions at $\sqrt{s_{{NN}}}$ = 193 GeV at STAR
DOI: 10.17182/hepdata.84821.v1/t6
title: "Figure 1A : 10-40% U+U collisions" of "Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\sqrt{s_{NN}}$ = 193 GeV at STAR"

description: The centrality dependence of e+e− invariant mass spectra within the STAR acceptance from Au+Au collisions and U+U collisions for pair pT &lt; 0.15 GeV/c. The vertical bars on data points depict the statistical uncertainties, while the systematic uncertainties are shown as gray boxes. The hadronic cocktail yields from U+U collisions are ∼5%–12% higher than those from Au+Au collisions in given centrality bins; thus only cocktails for Au+Au collisions are shown here as solid lines, with shaded bands representing the systematic uncertainties for clarity.
description: Low-pT e+e− pair production in Au+Au collisions at $\sqrt{s_{{NN}}}$ = 200 GeV and U+U collisions at $\sqrt{s_{{NN}}}$ = 193 GeV at STAR