cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79538.v1/t76
title: "X-section U.L. Gtc" of "Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector"

description: Upper limit cross-section, in femtobarn, for the $\tilde{g}\to t \tilde{t} \to t\tilde{\chi^{0}_{1}}+$soft grid.
description: A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\tilde{t}_1 \rightarrow t^{(*)} \tilde\chi^0_1$ and $\tilde{t}_1\rightarrow b\tilde\chi^\pm_1 \rightarrow b W^{(*)} \tilde\chi^0_1$, where $\tilde\chi^0_1$ ($\chi^\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \tilde\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\tilde\chi^0_1$ masses below 160 GeV. In the case where $m_{\tilde{t}_1}\sim m_t+m_{\tilde\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.
DOI: 10.17182/hepdata.79538.v1/t77
title: "SRAcutflowtable" of "Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector"

description: Cutflow for SRA for a signal model with top squark pair production in the case where both top squarks decay via $\tilde{t}_1\to t^{(*)} \tilde\chi^0_1$ with $m(\tilde{t}_1,\tilde\chi^0_1)=$ (800,1) GeV. An integrated luminosity of 36.1 $\mathrm{fb}^{-1}$ is assumed when calculating the weighted yields. For the derivation skim at least one of the following four criteria is required: $H_{\mathrm{T}}$ $&gt;$ 150 GeV; at least one loose electron with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two loose electrons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; at least one muon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two muons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; or at least one photon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two photons with $p_{\mathrm{T}}$ $&gt;$ 50 GeV.
description: A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\tilde{t}_1 \rightarrow t^{(*)} \tilde\chi^0_1$ and $\tilde{t}_1\rightarrow b\tilde\chi^\pm_1 \rightarrow b W^{(*)} \tilde\chi^0_1$, where $\tilde\chi^0_1$ ($\chi^\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \tilde\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\tilde\chi^0_1$ masses below 160 GeV. In the case where $m_{\tilde{t}_1}\sim m_t+m_{\tilde\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.
DOI: 10.17182/hepdata.79538.v1/t78
title: "SRBcutflowtable" of "Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector"

description: Cutflow SRB for a signal model with top squark pair production in the case where both top squarks decay via $\tilde{t}_1\to t^{(*)} \tilde\chi^0_1$ with $m(\tilde{t}_1,\tilde\chi^0_1)=$ (600,300) GeV. An integrated luminosity of 36.1 $\mathrm{fb}^{-1}$ is assumed when calculating the weighted yields. For the derivation skim at least one of the following four criteria is required: $H_{\mathrm{T}}$ $&gt;$ 150 GeV; at least one loose electron with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two loose electrons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; at least one muon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two muons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; or at least one photon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two photons with $p_{\mathrm{T}}$ $&gt;$ 50 GeV.
description: A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\tilde{t}_1 \rightarrow t^{(*)} \tilde\chi^0_1$ and $\tilde{t}_1\rightarrow b\tilde\chi^\pm_1 \rightarrow b W^{(*)} \tilde\chi^0_1$, where $\tilde\chi^0_1$ ($\chi^\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \tilde\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\tilde\chi^0_1$ masses below 160 GeV. In the case where $m_{\tilde{t}_1}\sim m_t+m_{\tilde\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.
DOI: 10.17182/hepdata.79538.v1/t79
title: "SRC12cutflowtable" of "Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector"

description: Cutflow for SRC1 and SRC2 for a signal model with top squark pair production in the case where both top squarks decay via $\tilde{t}_1\to t^{(*)} \tilde\chi^0_1$ with $m(\tilde{t}_1,\tilde\chi^0_1)=$ (250,77) GeV. An integrated luminosity of 36.1 $\mathrm{fb}^{-1}$ is assumed when calculating the weighted yields. For the derivation skim at least one of the following four criteria is required: $H_{\mathrm{T}}$ $&gt;$ 150 GeV; at least one loose electron with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two loose electrons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; at least one muon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two muons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; or at least one photon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two photons with $p_{\mathrm{T}}$ $&gt;$ 50 GeV.
description: A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\tilde{t}_1 \rightarrow t^{(*)} \tilde\chi^0_1$ and $\tilde{t}_1\rightarrow b\tilde\chi^\pm_1 \rightarrow b W^{(*)} \tilde\chi^0_1$, where $\tilde\chi^0_1$ ($\chi^\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \tilde\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\tilde\chi^0_1$ masses below 160 GeV. In the case where $m_{\tilde{t}_1}\sim m_t+m_{\tilde\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.
DOI: 10.17182/hepdata.79538.v1/t80
title: "SRC35cutflowtable" of "Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector"

description: Cutflow for SRC3, SRC4, and SRC5 for a signal model with top squark pair production in the case where both top squarks decay via $\tilde{t}_1\to t^{(*)} \tilde\chi^0_1$ with $m(\tilde{t}_1,\tilde\chi^0_1)=$ (500,327) GeV. An integrated luminosity of 36.1 $\mathrm{fb}^{-1}$ is assumed when calculating the weighted yields. For the derivation skim at least one of the following four criteria is required: $H_{\mathrm{T}}$ $&gt;$ 150 GeV; at least one loose electron with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two loose electrons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; at least one muon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two muons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; or at least one photon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two photons with $p_{\mathrm{T}}$ $&gt;$ 50 GeV.
description: A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\tilde{t}_1 \rightarrow t^{(*)} \tilde\chi^0_1$ and $\tilde{t}_1\rightarrow b\tilde\chi^\pm_1 \rightarrow b W^{(*)} \tilde\chi^0_1$, where $\tilde\chi^0_1$ ($\chi^\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \tilde\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\tilde\chi^0_1$ masses below 160 GeV. In the case where $m_{\tilde{t}_1}\sim m_t+m_{\tilde\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.
DOI: 10.17182/hepdata.79538.v1/t81
title: "SRDhighcutflowtable" of "Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector"

description: Cutflow for SRD-high for a signal model with bottom squark pair production in the case where both bottom squarks decay via $b\tilde\chi^{\pm}_1\to bW^{(*)} \tilde\chi^0_1$, with $m(\tilde\chi^{\pm}_1)-m(\tilde\chi^0_1) = 1$ GeV with $m(\tilde{t}_1,\tilde\chi^{\pm}_1)=$ (800,100) GeV. An integrated luminosity of 36.1 $\mathrm{fb}^{-1}$ is assumed when calculating the weighted yields. For the derivation skim at least one of the following four criteria is required: $H_{\mathrm{T}}$ $&gt;$ 150 GeV; at least one loose electron with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two loose electrons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; at least one muon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two muons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; or at least one photon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two photons with $p_{\mathrm{T}}$ $&gt;$ 50 GeV.
description: A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\tilde{t}_1 \rightarrow t^{(*)} \tilde\chi^0_1$ and $\tilde{t}_1\rightarrow b\tilde\chi^\pm_1 \rightarrow b W^{(*)} \tilde\chi^0_1$, where $\tilde\chi^0_1$ ($\chi^\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \tilde\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\tilde\chi^0_1$ masses below 160 GeV. In the case where $m_{\tilde{t}_1}\sim m_t+m_{\tilde\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.
DOI: 10.17182/hepdata.79538.v1/t83
title: "SREcutflowtable" of "Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector"

description: Cutflow for SRE for a signal model with gluino pair production in the case where both gluinos decay via $\tilde{g}\to t\tilde{t}_1\to t\tilde\chi^0_1+$soft and $\Delta m(\tilde{t}_1, \tilde\chi^0_1)=5$ GeV with $m(\tilde{g},\tilde{t}_1)=$ (1700,400) GeV. An integrated luminosity of 36.1 $\mathrm{fb}^{-1}$ is assumed when calculating the weighted yields. For the derivation skim at least one of the following four criteria is required: $H_{\mathrm{T}}$ $&gt;$ 150 GeV; at least one loose electron with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two loose electrons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; at least one muon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two muons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; or at least one photon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two photons with $p_{\mathrm{T}}$ $&gt;$ 50 GeV.
description: A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\tilde{t}_1 \rightarrow t^{(*)} \tilde\chi^0_1$ and $\tilde{t}_1\rightarrow b\tilde\chi^\pm_1 \rightarrow b W^{(*)} \tilde\chi^0_1$, where $\tilde\chi^0_1$ ($\chi^\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \tilde\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\tilde\chi^0_1$ masses below 160 GeV. In the case where $m_{\tilde{t}_1}\sim m_t+m_{\tilde\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.
DOI: 10.17182/hepdata.79538.v1/t82
title: "SRDlowcutflowtable" of "Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector"

description: Cutflow for SRD-low for a signal model with bottom squark pair production in the case where both bottom squarks decay via $b\tilde\chi^{\pm}_1\to bW^{(*)} \tilde\chi^0_1$, with $m(\tilde\chi^{\pm}_1)-m(\tilde\chi^0_1) = 1$ GeV witht $m(\tilde{t}_1,\tilde\chi^{\pm}_1)=$ (600,200) GeV. An integrated luminosity of 36.1 $\mathrm{fb}^{-1}$ is assumed when calculating the weighted yields. For the derivation skim at least one of the following four criteria is required: $H_{\mathrm{T}}$ $&gt;$ 150 GeV; at least one loose electron with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two loose electrons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; at least one muon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two muons with $p_{\mathrm{T}}$ $&gt;$ 20 GeV; or at least one photon with $p_{\mathrm{T}}$ $&gt;$ 100 GeV or at least two photons with $p_{\mathrm{T}}$ $&gt;$ 50 GeV.
description: A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\tilde{t}_1 \rightarrow t^{(*)} \tilde\chi^0_1$ and $\tilde{t}_1\rightarrow b\tilde\chi^\pm_1 \rightarrow b W^{(*)} \tilde\chi^0_1$, where $\tilde\chi^0_1$ ($\chi^\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \tilde\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\tilde\chi^0_1$ masses below 160 GeV. In the case where $m_{\tilde{t}_1}\sim m_t+m_{\tilde\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.
DOI: 10.17182/hepdata.79667.v1/t1
title: "Table 1" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The $v_{n}$ result from 2-particle correlation as a function of multiplicity ($N_{trk}^{offline}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Results after low-multiplicity subtraction are denoted as $v_{n}^{sub}$.
description: No data abstract available.
DOI: 10.17182/hepdata.79667.v1/t2
title: "Table 2" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The $v_{n}$ result from 2-particle correlation as a function of multiplicity ($N_{trk}^{offline}$) in pPb collisions at $\sqrt{s_{NN}}$ = 8.16 TeV. Results after low-multiplicity subtraction are denoted as $v_{n}^{sub}$.
description: No data abstract available.
DOI: 10.17182/hepdata.79667.v1/t3
title: "Table 3" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The $v_{4}$ result from 2-particle correlation as a function of multiplicity ($N_{trk}^{offline}$) in pp collisions at $\sqrt{s}$ = 13.00 TeV. Results after low-multiplicity subtraction are denoted as $v_{4}^{sub}$.
description: No data abstract available.
DOI: 10.17182/hepdata.79667.v1/t4
title: "Table 4" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.79667.v1/t5
title: "Table 5" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pPb collisions at $\sqrt{s_{NN}}$ = 8.16 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.79667.v1/t6
title: "Table 6" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pp collisions at $\sqrt{s}$ = 13.0 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.79667.v1/t7
title: "Table 7" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. The results are normalized by $\left&lt;(v_2^{\text{sub}})^{2}\right&gt; \, \left&lt;(v_3^{\text{sub}})^{2}\right&gt;$ and $\left&lt;(v_2^{\text{sub}})^{2}\right&gt; \, \left&lt;(v_4^{\text{sub}})^{2}\right&gt;$ from two-particle correlations.
description: No data abstract available.
DOI: 10.17182/hepdata.79667.v1/t8
title: "Table 8" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pPb collisions at $\sqrt{s_{NN}}$ = 8.16 TeV. The results are normalized by $\left&lt;(v_2^{\text{sub}})^{2}\right&gt; \, \left&lt;(v_3^{\text{sub}})^{2}\right&gt;$ and $\left&lt;(v_2^{\text{sub}})^{2}\right&gt; \, \left&lt;(v_4^{\text{sub}})^{2}\right&gt;$ from two-particle correlations.
description: No data abstract available.
DOI: 10.17182/hepdata.79667.v1/t9
title: "Table 9" of "Observation of correlated azimuthal anisotropy Fourier harmonics in pp and pPb collisions at the LHC"

description: The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pp collisions at $\sqrt{s}$ = 13.0 TeV. The results are normalized by $\left&lt;(v_2^{\text{sub}})^{2}\right&gt; \, \left&lt;(v_3^{\text{sub}})^{2}\right&gt;$ and $\left&lt;(v_2^{\text{sub}})^{2}\right&gt; \, \left&lt;(v_4^{\text{sub}})^{2}\right&gt;$ from two-particle correlations.
description: No data abstract available.
DOI: 10.17182/hepdata.79668.v1/t1
title: "Table 1" of "Observation of top quark production in proton-nucleus collisions"

description: Invariant mass distributions of the W candidate, $m_{jj'}$, in the 0 b category after all selections. The error bars indicate the statistical uncertainties.
description: Reconstructed invariant mass distributions of the hadronic W (jj') boson
and top quark (jj'b) candidates in each b jet category. The kinematic variables
describe the $\ell$+jets decay channel, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$). The measured cross sections are given per decay channel
and for their combination.

The fiducial region is defined as:
- $\equiv$1lepton, $p_T$&gt;30GeV&&|$\eta$|&lt;2.1
- exluding 1.444&lt;|$\eta$|&lt;1.566 region only in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;20GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;15GeV&&|$\eta$|&lt;2.4 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$4jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.5
- min($\Delta R(jet,\ell)$) &gt; 0.3
- ambiguities in pairing the jj' are resolved by choosing the combination that results in the smaller value of the $\Delta R(j,j')$, where $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$
- ambiguities in pairing the jj'b are resolved by choosing the combination that results in the smaller value of the $|m_{jj'b}-m_{\ell\nu b}|$

The acceptance is measured in the $\mu$+jets channel as:
0.060$\pm$0.002(tot)

The acceptance is measured in the $\rm{e}$+jets channel as:
0.056$\pm$0.002(tot)

The efficiency is measured in the $\mu$+jets channel as:
0.91$\pm$0.04(tot)

The efficiency is measured in the $\rm{e}$+jets channel as:
0.63$\pm$0.03(tot)
DOI: 10.17182/hepdata.79668.v1/t2
title: "Table 2" of "Observation of top quark production in proton-nucleus collisions"

description: Invariant mass distributions of the W candidate, $m_{jj'}$, in the 1 b category after all selections. The error bars indicate the statistical uncertainties.
description: Reconstructed invariant mass distributions of the hadronic W (jj') boson
and top quark (jj'b) candidates in each b jet category. The kinematic variables
describe the $\ell$+jets decay channel, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$). The measured cross sections are given per decay channel
and for their combination.

The fiducial region is defined as:
- $\equiv$1lepton, $p_T$&gt;30GeV&&|$\eta$|&lt;2.1
- exluding 1.444&lt;|$\eta$|&lt;1.566 region only in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;20GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;15GeV&&|$\eta$|&lt;2.4 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$4jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.5
- min($\Delta R(jet,\ell)$) &gt; 0.3
- ambiguities in pairing the jj' are resolved by choosing the combination that results in the smaller value of the $\Delta R(j,j')$, where $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$
- ambiguities in pairing the jj'b are resolved by choosing the combination that results in the smaller value of the $|m_{jj'b}-m_{\ell\nu b}|$

The acceptance is measured in the $\mu$+jets channel as:
0.060$\pm$0.002(tot)

The acceptance is measured in the $\rm{e}$+jets channel as:
0.056$\pm$0.002(tot)

The efficiency is measured in the $\mu$+jets channel as:
0.91$\pm$0.04(tot)

The efficiency is measured in the $\rm{e}$+jets channel as:
0.63$\pm$0.03(tot)