cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.82211.v1/t7
title: "Table 7" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: The MiniBooNE $\bar{\nu}_\mu$ CCQE double-differential cross section, with the shape uncertainty, on carbon. The units are fb/GeV $(10^{-39} \mbox{cm}^2/\mbox{GeV})$. Not included in the table is the total normalization uncertainty of 17.4%.
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82211.v1/t8
title: "Table 8" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: The QE-like $\bar{\nu}_\mu$ background subtracted from the double-differential cross section on carbon. The $\bar{\nu}_\mu$ CCQE interactions with hydrogen are treated as background in this calculation, and so their contribution is included here. The units are fb/GeV $(10^{-39} \mbox{cm}^2/\mbox{GeV})$ .
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82211.v1/t10
title: "Table 10" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: The MiniBooNE $\bar{\nu}_\mu$ CCQE total cross section on carbon, total and shape errors, and predicted CCQE-like background in bins of $E_\nu^{\textrm{QE,RFG}}$ and units of fb $(10^{-39} \mbox{cm}^2)$. The total error includes both the shape and normalization uncertainties.
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82211.v1/t9
title: "Table 9" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: The MiniBooNE $\bar{\nu}_\mu$ CCQE single differential cross section $\frac{d\sigma}{dQ^2_{QE}}$ on carbon, shape error, and CCQE-like background in units of fb/GeV$^2$ $(10^{-39} \mbox{cm}^2/\mbox{GeV}^2)$ . The $\bar{\nu}_\mu$ CCQE content is treated as background. Not included in the table is the total normalization error of 17.4%.
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82212.v1/t1
title: "Table 1" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Distribution of m<sub>T2</sub> in the signal region of the lep-had channel before the respective selection requirements, indicated by the vertical line and arrow, are applied. The stacked histograms show the various SM background contributions. The total background from events with a fake tau lepton in the lep-had channel (fake τ<sub>had</sub> + e /μ) is obtained from the fake-factor method. The hatched band indicates the total statistical and systematic uncertainty in the SM background. The error bars on the black data points represent the statistical uncertainty in the data yields. The dashed line shows the expected additional yields from a benchmark signal model. The rightmost bin includes the overflow.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t2
title: "Table 2" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Distributions of E<sub>T</sub><sup>miss</sup> in the signal region of the lep-had channel before the respective selection requirements, indicated by the vertical line and arrow, are applied. The stacked histograms show the various SM background contributions. The total background from events with a fake tau lepton in the lep-had channel (fake τ<sub>had</sub> + e /μ) is obtained from the fake-factor method. The hatched band indicates the total statistical and systematic uncertainty in the SM background. The error bars on the black data points represent the statistical uncertainty in the data yields. The dashed line shows the expected additional yields from a benchmark signal model. The rightmost bin includes the overflow.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t3
title: "Table 3" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Distributions of m<sub>T2</sub> in the signal region of the had-had channel before the respective selection requirements, indicated by the vertical line and arrow, are applied. Here, τ<sub>1</sub> (τ<sub>2</sub>) refers to the leading (subleading) τ<sub>had</sub>. The stacked histograms show the various SM background contributions. The hatched band indicates the total statistical and systematic uncertainty in the SM background. The error bars on the black data points represent the statistical uncertainty in the data yields. The dashed line shows the expected additional yields from a benchmark signal model. The rightmost bin includes the overflow.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t4
title: "Table 4" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Distributions of E<sub>T</sub><sup>miss</sup> in the signal region of the had-had channel before the respective selection requirements, indicated by the vertical line and arrow, are applied. Here, τ<sub>1</sub> (τ<sub>2</sub>) refers to the leading (subleading) τ<sub>had</sub>. The stacked histograms show the various SM background contributions. The hatched band indicates the total statistical and systematic uncertainty in the SM background. The error bars on the black data points represent the statistical uncertainty in the data yields. The dashed line shows the expected additional yields from a benchmark signal model. The rightmost bin includes the overflow.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t10
title: "Table 10" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Signal acceptance A in percent for the signal region of the lep-had channel. The signal acceptance A is determined from a generator-level implementation of the analysis. It includes the branching ratios for the decays of the tau leptons. The selection efficiency ε is calculated using reconstructed objects, i.e. including all detector effects, and defined such that the event yields in the signal regions are given by the product A · ε · N<sub>signal</sub>, where N<sub>signal</sub> = σ · 36.1 fb<sup>-1</sup> and σ is the theoretical prediction for the production cross section of top-squark pairs with the mass given on the horizontal axis.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t5
title: "Table 5" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: <b>Exclusion contour (obs)</b> Expected (solid blue line) and observed (solid red line) exclusion-limit contours at 95% confidence level in the plane of top-squark and tau-slepton mass for the simplified model, obtained from the statistical combination of the lep-had and had-had channels, using full experimental and theory systematic uncertainties except the theoretical uncertainty in the signal cross section. The yellow band shows one-standard-deviation variations around the expected limit contour. The dotted red lines indicate how the observed limit moves when varying the signal cross section up or down by the corresponding uncertainty in the theoretical value. For comparison, the plot also shows the observed exclusion contour from the ATLAS Run-1 analysis as the area shaded in gray and the limit on the mass of the tau slepton (for a massless LSP) from the LEP experiments as a green band.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t6
title: "Table 6" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: <b>Exclusion contour (exp)</b> Expected (solid blue line) and observed (solid red line) exclusion-limit contours at 95% confidence level in the plane of top-squark and tau-slepton mass for the simplified model, obtained from the statistical combination of the lep-had and had-had channels, using full experimental and theory systematic uncertainties except the theoretical uncertainty in the signal cross section. The yellow band shows one-standard-deviation variations around the expected limit contour. The dotted red lines indicate how the observed limit moves when varying the signal cross section up or down by the corresponding uncertainty in the theoretical value. For comparison, the plot also shows the observed exclusion contour from the ATLAS Run-1 analysis as the area shaded in gray and the limit on the mass of the tau slepton (for a massless LSP) from the LEP experiments as a green band.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t7
title: "Table 7" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Expected numbers of events from the SM background processes from the background fit and observed event yield in data for the signal regions in the lep-had and had-had channel, given for an integrated luminosity of 36.1 fb<sup>-1</sup>. The expected yield for the signal model with m(t̃<sub>1</sub>)=1100 GeV and m(τ̃<sub>1</sub>)=590 GeV is shown for comparison. The uncertainties include both the statistical and systematic uncertainties and are truncated at zero. The total background from events with a fake tau lepton in the lep-had channel (fake τ<sub>had</sub> + e /μ) is obtained from the fake-factor method.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t8
title: "Table 8" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Normalization factors obtained from the background-only fit. The normalization factor for tt̄ events with fake tau leptons is only relevant for the had-had channel.
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.
DOI: 10.17182/hepdata.82212.v1/t9
title: "Table 9" of "Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Left to right: observed 95% CL upper limits on the visible cross section (〈 A ε σ 〉<sub>obs</sub><sup>95</sup>) and on the number of signal events (S<sub>obs</sub><sup>95</sup> ). The third column (S<sub>exp</sub><sup>95</sup>) shows the expected 95% CL upper limit on the number of signal events, given the expected number (and ± 1σ excursions on the expectation) of background events. The last two columns indicate the CL<sub>b</sub> value, i.e. the confidence level observed for the background-only hypothesis, and the discovery p-value (p(s = 0)) and the corresponding significance (Z).
description: A search for direct pair production of top squarks in final states with two tau leptons, $b$-jets, and missing transverse momentum is presented. The analysis is based on proton--proton collision data at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of 36.1/fb recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. Two exclusive channels with either two hadronically decaying tau leptons or one hadronically and one leptonically decaying tau lepton are considered. No significant deviation from the Standard Model predictions is observed in the data. The analysis results are interpreted in terms of model-independent limits and used to derive exclusion limits on the masses of the top squark $\tilde t_1$ and the tau slepton $\tilde \tau_1$ in a simplified model of Supersymmetry with a nearly massless gravitino. In this model, masses up to $m(\tilde t_1) =$ 1.16 TeV and $m(\tilde \tau_1) =$ 1.00 TeV are excluded at 95\% confidence level.