cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.84426.v2/t37
title: "X-section U.L. 1" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Observed upper limits on the production cross section at 95% CL in pb as a function of the LSP mass and the gluino mass.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t38
title: "Yieldtable 1" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Yields of the expected background from the SM in the bins of the multibin SR of the $2\tau$ channel with all bins being simultaneously used to constrain the background prediction. Expectation is given with the scalings computed in the combined fit applied. Uncertainties are statistial plus systematrics. Only the subsamples contributing the respective region are considered.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t39
title: "VR kinematics 1" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $m_{\mathrm{T}}^{\tau}$ in the compressed $m_{\mathrm{T}}^{\tau}$ VR of the $1\tau$ channel, illustrating the background modeling after the fit. The last bin includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t40
title: "VR kinematics 2" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $E_{\mathrm{T}}^{\mathrm{miss}}$ in the compressed $E_{\mathrm{T}}^{\mathrm{miss}}$ VR of the $1\tau$ channel, illustrating the background modeling after the fit. The last bin includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t41
title: "VR kinematics 3" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $m_{\mathrm{T}}^{\tau}$ in the medium-mass $m_{\mathrm{T}}^{\tau}$ VR of the $1\tau$ channel, illustrating the background modeling after the fit. The last bin includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t42
title: "VR kinematics 4" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $E_{\mathrm{T}}^{\mathrm{miss}}$ in the medium-mass $E_{\mathrm{T}}^{\mathrm{miss}}$ VR of the $1\tau$ channel, illustrating the background modeling after the fit. The last bin includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t43
title: "VR kinematics 5" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $H_{\mathrm{T}}$ in the medium-mass $H_{\mathrm{T}}$ VR of the $1\tau$ channel, illustrating the background modeling after the fit. The last bin includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t44
title: "VR kinematics 6" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $m_{\mathrm{T}}^{\tau_1}$ + $m_{\mathrm{T}}^{\tau_2}$ in the top VR of the $2\tau$ channel, illustrating the background modeling after the fit. The last bin includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t45
title: "VR kinematics 7" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $H_{\mathrm{T}}$ in the $W$ VR of the $2\tau$ channel, illustrating the background modeling after the fit. The last bin includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t46
title: "VR kinematics 8" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $m_{\mathrm{T}}^{\tau_1}$ + $m_{\mathrm{T}}^{\tau_2}$ in the $Z$ VR of the $2\tau$ channel, illustrating the background modeling after the fit. The last bin includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t47
title: "N-1 SR kinematics 1" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $m_{\mathrm{T}}^{\tau}$ in the compressed SR of the $1\tau$ channel before application of the $m_{\mathrm{T}}^{\tau}$ &gt; 80 GeV requirement. The last bin includes overflow events. Signal predictions corresponding to the simplified model scenarios of low (LM), medium (MM), and high mass-splitting (HM) as well as for the GMSB benchmark are given.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t48
title: "N-1 SR kinematics 2" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $H_{\mathrm{T}}$ in the medium-mass SR of the $1\tau$ channel before application of the $H_{\mathrm{T}}$ &gt; 1000 GeV requirement. The last bin includes overflow events. Signal predictions corresponding to the simplified model scenarios of low (LM), medium (MM), and high mass-splitting (HM) as well as for the GMSB benchmark are given.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t49
title: "N-1 SR kinematics 3" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $m_{\mathrm{T}}^{\mathrm{sum}}$ in the compressed SR of the $2\tau$ channel before application of the $m_{\mathrm{T}}^{\mathrm{sum}}$ &gt; 1600 GeV requirement. The last bin includes overflow events. Signal predictions corresponding to the simplified model scenarios of low (LM), medium (MM), and high mass-splitting (HM) as well as for the GMSB benchmark are given.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t50
title: "N-1 SR kinematics 4" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $H_{\mathrm{T}}$ in the high-mass SR of the $2\tau$ channel before application of the $H_{\mathrm{T}}$ &gt; 1100 GeV requirement. The last bin includes overflow events. Signal predictions corresponding to the simplified model scenarios of low (LM), medium (MM), and high mass-splitting (HM) as well as for the GMSB benchmark are given.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t51
title: "SR kinematics 1" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: mT(tau_1) + mT(tau_2) in the multibin SR of the 2T channel. The last bin includes overflow events. Signal predictions corresponding to the simplified model scenarios of low (LM), medium (MM), and high mass-splitting (HM) as well as for the GMSB benchmark are given.
description: No data abstract available.
DOI: 10.17182/hepdata.84426.v2/t52
title: "N-1 SR kinematics 5" of "Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: $H_{\mathrm{T}}$ in the GMSB SR of the $2\tau$ channel before application of the $H_{\mathrm{T}}$ &gt; 1900 GeV requirement. The last bin includes overflow events. Signal predictions corresponding to the simplified model scenarios of low (LM), medium (MM), and high mass-splitting (HM) as well as for the GMSB benchmark are given.
description: No data abstract available.
DOI: 10.17182/hepdata.84584.v3/t1
title: "Table 1" of "Measurement of antiproton production in ${\rm p He}$ collisions at $\sqrt{s_{NN}}=110$ GeV"

description: Double-differential cross-section in antiproton momentum and transverse momentum for antiproton production in collisions of 6.5 TeV protons on He nuclei at rest. The antiproton momentum is defined in the laboratory frame. Results are averaged over the given kinematic range of each bin. The uncertainty is split into an uncertainty delta_uncorr, uncorrelated among the kinematic bins, and an uncertainty delta_corr, fully correlated among the kinematic bins. For both uncertainties, the systematic uncertainty, dominant for most bins, and the statistical uncertainty, are added in quadrature. The average value within each bin is also reported for the antiproton momentum, the transverse momentum. These average values are obtained from simulation (based on EPOS LHC), to avoid biases from reconstruction effects and given the good agreement with data observed for the simulated kinematic spectra. Projections of Table1 distribution in antiproton $p_T$ bins.
description: No data abstract available.
DOI: 10.17182/hepdata.84584.v3/t2
title: "Table 2" of "Measurement of antiproton production in ${\rm p He}$ collisions at $\sqrt{s_{NN}}=110$ GeV"

description: The average value of antiproton x-Feynman $x_F=2 p_{Z}^{*}/\sqrt{s}$ in bins of antiproton momentum and transverse momentum in collisions of 6.5 TeV protons on He nuclei at rest, where $p_{Z}^{*}$ is the longitudinal antiproton momentum in the center-of-mass system and $\sqrt{s}$ the nucleon-nucleon center-of-mass energy. In each bin the average value is reported for the antiproton momentum and transverse momentum. These average values are obtained from simulation (based on EPOS LHC), to avoid biases from reconstruction effects and given the good agreement with data observed for the simulated kinematic spectra. Projections of Table 3 distribution in antiproton $p_T$ bins.
description: No data abstract available.
DOI: 10.17182/hepdata.84584.v1/t1
title: "Table 1" of "Measurement of antiproton production in ${\rm p He}$ collisions at $\sqrt{s_{NN}}=110$ GeV"

description: Double-differential cross-section in antiproton momentum and transverse momentum for antiproton production in collisions of 6.5 TeV protons on He nuclei at rest. The antiproton momentum is defined in the laboratory frame. Results are averaged over the given kinematic range of each bin. The uncertainty is split into an uncertainty delta_uncorr, uncorrelated among the kinematic bins, and an uncertainty delta_corr, fully correlated among the kinematic bins. For both uncertainties, the systematic uncertainty, dominant for most bins, and the statistical uncertainty, are added in quadrature. The average value within each bin is also reported for the antiproton momentum, the transverse momentum, and x-Feynman xF=2 p_Z*/SQRT(S), where p_Z* is the longitudinal antiproton momentum in the center-of-mass system and SQRT(S) the nucleon-nucleon center-of-mass energy. These average values are obtained from simulation (based on EPOS LHC), to avoid biases from reconstruction effects and given the good agreement with data observed for the simulated kinematic spectra.
description: No data abstract available.
DOI: 10.17182/hepdata.84584.v2/t1
title: "Table 1" of "Measurement of antiproton production in ${\rm p He}$ collisions at $\sqrt{s_{NN}}=110$ GeV"

description: Double-differential cross-section in antiproton momentum and transverse momentum for antiproton production in collisions of 6.5 TeV protons on He nuclei at rest. The antiproton momentum is defined in the laboratory frame. Results are averaged over the given kinematic range of each bin. The uncertainty is split into an uncertainty delta_uncorr, uncorrelated among the kinematic bins, and an uncertainty delta_corr, fully correlated among the kinematic bins. For both uncertainties, the systematic uncertainty, dominant for most bins, and the statistical uncertainty, are added in quadrature. The average value within each bin is also reported for the antiproton momentum, the transverse momentum, and x-Feynman xF=2 p_Z*/SQRT(S), where p_Z* is the longitudinal antiproton momentum in the center-of-mass system and SQRT(S) the nucleon-nucleon center-of-mass energy. These average values are obtained from simulation (based on EPOS LHC), to avoid biases from reconstruction effects and given the good agreement with data observed for the simulated kinematic spectra.
description: No data abstract available.
DOI: 10.17182/hepdata.84597.v1/t1
title: "Table 1" of "Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at sqrt(s)=13 TeV"

description: Data, estimated background and uncertainties, in the region defined by |y*|&lt;0.3.
description: Searches for dijet resonances with sub-TeV masses using the ATLAS detector at the Large Hadron Collider can be statistically limited by the bandwidth available to inclusive single-jet triggers, whose data-collection rates at low transverse momentum are much lower than the rate from Standard Model multijet production. This data refers to a search for dijet resonances using a strategy called "Trigger-object Level Analysis" (TLA) in ATLAS, where the limitation on high-rate events that can be used for the search is overcome by recording only the event information calculated by the jet trigger algorithms, thereby allowing much higher event rates with reduced storage needs.
There are two event selections leading to two signal regions in the search, one with |y*| &lt; 0.3 and one with |y*| &lt; 0.6. The definition of y* is (y1-y2)/2, where y1 and y2 are the rapidities of the highest- and second-highest-pT trigger-level jets.
The event selection for the |y*| &lt; 0.3 region is:
- highest-pT-jet &gt; 185 GeV
- second-highest-pT-jet &gt; 85 GeV
- dijet invariant mass &gt; 400 GeV
- |y*| &lt; 0.3
The event selection for the |y*| &lt; 0.6 region is:
- highest-pT-jet &gt; 220 GeV
- second-highest-pT-jet &gt; 85 GeV
- dijet invariant mass &gt; 531 GeV
- |y*| &lt; 0.6
The background is calculated using two different fit functions, using a sliding window algorithm described in the paper. The systematic uncertainties on the background account for the choice of the fit function (called "sys, fit function") and for the uncertainties on the fit parameters due to the statistical error of the data (called "sys, fit parameters"). The fit function uncertainty is a one-sided systematic uncertainty. No significant excess with respect to the background prediction is found in the data. The results is interpreted in the paper in terms of a leptophobic mediator of dark matter as in arXiv:1507.00966, here we report the 95% CL limit on Gaussian-shaped resonant processes that can be used to constrain generic resonant processes as described in Appendix A of arXiv:1407.1376.
DOI: 10.17182/hepdata.84597.v1/t2
title: "Table 2" of "Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at sqrt(s)=13 TeV"

description: Data, estimated background and uncertainties, in the region defined by |y*|&lt;0.6.
description: Searches for dijet resonances with sub-TeV masses using the ATLAS detector at the Large Hadron Collider can be statistically limited by the bandwidth available to inclusive single-jet triggers, whose data-collection rates at low transverse momentum are much lower than the rate from Standard Model multijet production. This data refers to a search for dijet resonances using a strategy called "Trigger-object Level Analysis" (TLA) in ATLAS, where the limitation on high-rate events that can be used for the search is overcome by recording only the event information calculated by the jet trigger algorithms, thereby allowing much higher event rates with reduced storage needs.
There are two event selections leading to two signal regions in the search, one with |y*| &lt; 0.3 and one with |y*| &lt; 0.6. The definition of y* is (y1-y2)/2, where y1 and y2 are the rapidities of the highest- and second-highest-pT trigger-level jets.
The event selection for the |y*| &lt; 0.3 region is:
- highest-pT-jet &gt; 185 GeV
- second-highest-pT-jet &gt; 85 GeV
- dijet invariant mass &gt; 400 GeV
- |y*| &lt; 0.3
The event selection for the |y*| &lt; 0.6 region is:
- highest-pT-jet &gt; 220 GeV
- second-highest-pT-jet &gt; 85 GeV
- dijet invariant mass &gt; 531 GeV
- |y*| &lt; 0.6
The background is calculated using two different fit functions, using a sliding window algorithm described in the paper. The systematic uncertainties on the background account for the choice of the fit function (called "sys, fit function") and for the uncertainties on the fit parameters due to the statistical error of the data (called "sys, fit parameters"). The fit function uncertainty is a one-sided systematic uncertainty. No significant excess with respect to the background prediction is found in the data. The results is interpreted in the paper in terms of a leptophobic mediator of dark matter as in arXiv:1507.00966, here we report the 95% CL limit on Gaussian-shaped resonant processes that can be used to constrain generic resonant processes as described in Appendix A of arXiv:1407.1376.
DOI: 10.17182/hepdata.84597.v1/t3
title: "Table 3" of "Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at sqrt(s)=13 TeV"

description: Observed 95% CL limit on cross section times acceptance times branching ratio for each width and mass of Gaussian signal shape tested, in the region defined by |y*|&lt;0.3.
description: Searches for dijet resonances with sub-TeV masses using the ATLAS detector at the Large Hadron Collider can be statistically limited by the bandwidth available to inclusive single-jet triggers, whose data-collection rates at low transverse momentum are much lower than the rate from Standard Model multijet production. This data refers to a search for dijet resonances using a strategy called "Trigger-object Level Analysis" (TLA) in ATLAS, where the limitation on high-rate events that can be used for the search is overcome by recording only the event information calculated by the jet trigger algorithms, thereby allowing much higher event rates with reduced storage needs.
There are two event selections leading to two signal regions in the search, one with |y*| &lt; 0.3 and one with |y*| &lt; 0.6. The definition of y* is (y1-y2)/2, where y1 and y2 are the rapidities of the highest- and second-highest-pT trigger-level jets.
The event selection for the |y*| &lt; 0.3 region is:
- highest-pT-jet &gt; 185 GeV
- second-highest-pT-jet &gt; 85 GeV
- dijet invariant mass &gt; 400 GeV
- |y*| &lt; 0.3
The event selection for the |y*| &lt; 0.6 region is:
- highest-pT-jet &gt; 220 GeV
- second-highest-pT-jet &gt; 85 GeV
- dijet invariant mass &gt; 531 GeV
- |y*| &lt; 0.6
The background is calculated using two different fit functions, using a sliding window algorithm described in the paper. The systematic uncertainties on the background account for the choice of the fit function (called "sys, fit function") and for the uncertainties on the fit parameters due to the statistical error of the data (called "sys, fit parameters"). The fit function uncertainty is a one-sided systematic uncertainty. No significant excess with respect to the background prediction is found in the data. The results is interpreted in the paper in terms of a leptophobic mediator of dark matter as in arXiv:1507.00966, here we report the 95% CL limit on Gaussian-shaped resonant processes that can be used to constrain generic resonant processes as described in Appendix A of arXiv:1407.1376.
DOI: 10.17182/hepdata.84597.v1/t4
title: "Table 4" of "Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at sqrt(s)=13 TeV"

description: Expected 95% CL limit on cross section times acceptance times branching ratio for each width and mass of Gaussian signal shape tested, in the region defined by |y*|&lt;0.3.
description: Searches for dijet resonances with sub-TeV masses using the ATLAS detector at the Large Hadron Collider can be statistically limited by the bandwidth available to inclusive single-jet triggers, whose data-collection rates at low transverse momentum are much lower than the rate from Standard Model multijet production. This data refers to a search for dijet resonances using a strategy called "Trigger-object Level Analysis" (TLA) in ATLAS, where the limitation on high-rate events that can be used for the search is overcome by recording only the event information calculated by the jet trigger algorithms, thereby allowing much higher event rates with reduced storage needs.
There are two event selections leading to two signal regions in the search, one with |y*| &lt; 0.3 and one with |y*| &lt; 0.6. The definition of y* is (y1-y2)/2, where y1 and y2 are the rapidities of the highest- and second-highest-pT trigger-level jets.
The event selection for the |y*| &lt; 0.3 region is:
- highest-pT-jet &gt; 185 GeV
- second-highest-pT-jet &gt; 85 GeV
- dijet invariant mass &gt; 400 GeV
- |y*| &lt; 0.3
The event selection for the |y*| &lt; 0.6 region is:
- highest-pT-jet &gt; 220 GeV
- second-highest-pT-jet &gt; 85 GeV
- dijet invariant mass &gt; 531 GeV
- |y*| &lt; 0.6
The background is calculated using two different fit functions, using a sliding window algorithm described in the paper. The systematic uncertainties on the background account for the choice of the fit function (called "sys, fit function") and for the uncertainties on the fit parameters due to the statistical error of the data (called "sys, fit parameters"). The fit function uncertainty is a one-sided systematic uncertainty. No significant excess with respect to the background prediction is found in the data. The results is interpreted in the paper in terms of a leptophobic mediator of dark matter as in arXiv:1507.00966, here we report the 95% CL limit on Gaussian-shaped resonant processes that can be used to constrain generic resonant processes as described in Appendix A of arXiv:1407.1376.