cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77603.v1/t19
title: "Table 19" of "Azimuthal anisotropy of charged particles with transverse momentum up to 100 GeV in PbPb collisions at sqrt(s[NN]) = 5.02 TeV"

description: The $v_{2}$ result from 4-, 6- and 8-particle cumulant methods as a function of $p_{T}$ in 40-50\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.77603.v1/t20
title: "Table 20" of "Azimuthal anisotropy of charged particles with transverse momentum up to 100 GeV in PbPb collisions at sqrt(s[NN]) = 5.02 TeV"

description: The $v_{2}$ result from 4-, 6- and 8-particle cumulant methods as a function of $p_{T}$ in 50-60\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.77603.v1/t21
title: "Table 21" of "Azimuthal anisotropy of charged particles with transverse momentum up to 100 GeV in PbPb collisions at sqrt(s[NN]) = 5.02 TeV"

description: The $v_{2}^{high}$ as a function of $v_{2}^{low}$ results from SP method in PbPb collisions at $sqrt{s_{NN}}$ = 5.02 TeV. Only statistical uncertainties are shown.
description: No data abstract available.
DOI: 10.17182/hepdata.77603.v1/t22
title: "Table 22" of "Azimuthal anisotropy of charged particles with transverse momentum up to 100 GeV in PbPb collisions at sqrt(s[NN]) = 5.02 TeV"

description: The $v_{2}^{high}$ as a function of $v_{2}^{low}$ results from 4-particle cumulant method in PbPb collisions at $sqrt{s_{NN}}$ = 5.02 TeV. Only statistical uncertainties are shown.
description: No data abstract available.
DOI: 10.17182/hepdata.77606.v1/t1
title: "Table 2" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Summary of the lower bounds of the first and final bins in $H_{\mathrm{T}}$ in [GeV] (the latter in parentheses) as a function of $n_{\text{jet}}$ and $n_{\text{b}}$.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t2
title: "Table 3" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Systematic uncertainties (in percent) in the transfer ($\mathcal{T}$) factors used in the method to estimate the SM backgrounds with genuine $\vec{p}_t^{miss}$ in the signal region. The quoted ranges provide representative values of the observed variations as a function of $n_{\mathrm{jet}}$ and $H_{\mathrm{T}}$.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t20
title: "Additional Figure 22" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Covariance matrix for the SM background estimates obtained using the simplified binning scheme, determined from a simultaneous fit to data in the control regions only (CR-only fit). The uncertainties in the background estimates are correlated in such a way that the covariance is typically positive. Small positive values, as well as the few negative values, are not shown.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t22
title: "Additional Table 1" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Observed data counts and "post-fit" background expectations based on the result of a combined fit to the signal region and multiple control regions under the SM-only hypothesis for the "monojet" event category. The rows labelled SM "pre-fit' show the background expectations when excluding the signal region from the fit. The uncertainties include statistical as well as systematic contributions.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t3
title: "Table 4" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: A summary of the simplified SUSY models used to interpret the results of this search. All on-shell SUSY particles in the decay are stated.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t4
title: "Table 5" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: A summary of benchmark simplified models, the most sensitive $n_{\mathrm{jet}}$ categories, and representative values for the corresponding experimental acceptance times efficiency ($\mathcal{A}\varepsilon$), the dominant systematic uncertainties, the theoretical production cross section ($\sigma_{\mathrm{theory}}$), and the expected and observed upper limits on the production cross section, expressed in terms of the signal strength parameter ($\mu$).
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t5
title: "Table 6" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Summary of the mass limits obtained for the fourteen classes of simplified models. The limits indicate the strongest observed and expected (in parentheses) mass exclusions in $\tilde{g}$, $\tilde{q}$, $\tilde{b}$, $\tilde{t}$, and $\tilde{\chi}_1^0$. The quoted values have uncertainties of $\pm 25$ and $\pm 10$ GeV for models involving the pair production of, respectively, gluinos and squarks.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t15
title: "Additional Figure 2, Expected" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the expected exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t23
title: "Additional Table 2" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Observed data counts and "post-fit" background expectations based on the result of a combined fit to the signal region and multiple control regions under the SM-only hypothesis for the "asymmetric" event categories. The rows labelled SM "pre-fit" show the background expectations when excluding the signal region from the fit. The uncertainties include statistical as well as systematic contributions.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t25
title: "Additional Table 4" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Summary of a simplified binning scheme comprising $H_{\mathrm{T}}^{\mathrm{miss}}$ shapes for eight representative event topologies, defined in terms of requirements on $n_{\mathrm{jet}}$ both symmetric and asymmetric categories) and $n_{\mathrm{b}}$. For each topology, event yields are integrated over the full $H_{\mathrm{T}}$ range, $H_{\mathrm{T}} &gt; 200$ GeV, and are categorised according to eight bins in $H_{\mathrm{T}}^{\mathrm{miss}}$ -- $130 &lt; H_{\mathrm{T}}^{\mathrm{miss}} &lt; 200$ GeV, six bins 100 GeV wide in the region $200 &lt; H_{\mathrm{T}}^{\mathrm{miss}} &lt; 800$ GeV, and an open final bin, $H_{\mathrm{T}}^{\mathrm{miss}} &gt; 800$ GeV. This categorisation scheme leads to 64 bins that are exclusive, contiguous, and provide complete coverage of the signal region. The corresponding SM background estimates for these 64 bins are obtained using the nominal likelihood model. The $H_{\mathrm{T}}^{\mathrm{miss}}$ template for each topology is determined from simulation and the normalisation for each template is given by an aggregate of estimates from several ($n_{\mathrm{jet}}$, $n_{\mathrm{b}}$, $H_{\mathrm{T}}$) bins, defined according to the nominal binning scheme.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t26
title: "Additional Table 5" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Observed data yields and "CR-only fit" SM background expectations using the simplified binning scheme, as a function of topology and $H_{\mathrm{T}}^{\mathrm{miss}}$. The SM backgrounds are determined from a simultaneous fit to data in the control regions. The data yields in the signal region are masked and excluded from the fit. The uncertainties include statistical as well as systematic contributions.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t18
title: "Additional Figure 2, Observed" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the observed exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t21
title: "Additional Figure 3, Expected" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the expected exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t24
title: "Additional Figure 3, Observed" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the observed exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t27
title: "Additional Figure 4, Expected" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the expected exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t30
title: "Additional Figure 4, Observed" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the observed exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t33
title: "Additional Figure 5, Expected" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1tttt model. This line is the expected exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t36
title: "Additional Figure 5, Observed" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1tttt model. This line is the observed exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t39
title: "Additional Figure 6, Expected" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1ttbb model. This line is the expected exclusion.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t42
title: "Additional Figure 2, Expected ($+1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t43
title: "Additional Figure 2, Expected ($-1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t44
title: "Additional Figure 2, Observed ($+1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t45
title: "Additional Figure 2, Observed ($-1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t46
title: "Additional Figure 3, Expected ($+1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t47
title: "Additional Figure 3, Expected ($-1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t48
title: "Additional Figure 3, Observed ($+1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t49
title: "Additional Figure 3, Observed ($-1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).
DOI: 10.17182/hepdata.77606.v1/t50
title: "Additional Figure 4, Expected ($+1\sigma$)" of "A search for new phenomena in pp collisions at sqrt(s) = 13 TeV in final states with missing transverse momentum and at least one jet using the alphaT variable"

description: Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.
description: CERN-LHC. A search for new phenomena in pp collisions at $\sqrt{s} = 13$ TeV in final states with missing transverse momentum and at least one jet using the $\alpha_{\mathrm{T}}$ variable. The final states are multiple jets and missing transverse momentum (MET).