cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.81690.v1/t1
title: "Table 1" of "Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton"

description: The measured fiducial cross sections in the $\ell$+jets and dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels. The first uncertainty is the statistical, the second is the systematic, and the last due to the integrated luminosity.
description: The kinematic variables
describe the $\ell$+jets, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$), and the dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels.
The measured cross sections are given per decay channel and for their combination.

The fiducial region in the $\ell$+jets decay channel is defined as:
- $\equiv$1$\rm{e}$($\mu$), $p_T$&gt;35(25)GeV&&|$\eta$|&lt;2.1
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;15GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;10GeV&&|$\eta$|&lt;2.5 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.4
- 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 $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$

The acceptance is measured in the $\ell$+jets channel as:
0.301$\pm$0.007(tot)

The fiducial region in the dilepton decay channel is defined as: 
- $\geq1\rm{e}$ or $\mu$ with $p_T$&gt;20GeV&&|$\eta$|&lt;2.4 and $p_T$&gt;18GeV&&|$\eta$|&lt;2.1, respectively
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region for electrons
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;3.0
- min($\Delta R(jet,\ell)$) &gt; 0.3
- $M_{\ell \ell}$ &gt; 20 GeV
- 76 &lt;$M_{\ell \ell}$ &lt; 106 GeV and $p_{\rm{T}}^{\rm{mss}}$&gt;35 GeV only in the $\mu^\pm \mu^\mp$ channel
- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum

The acceptance is measured in the dilepton channel as:
0.53$\pm$0.01(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.37$\pm$0.01(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

The efficiency is measured in the dilepton channel as:
0.55$\pm$0.02(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.57$\pm$0.04(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

In both the $\ell$+jets and dilepton analyses, events with $\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.
DOI: 10.17182/hepdata.81690.v1/t2
title: "Table 2" of "Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton"

description: The measured total cross sections based on the $\ell$+jets (left), $\rm{e}^\pm \mu^\mp$ (middle) and $\mu^\pm \mu^\mp$ (right) decay channels. The first uncertainty is the statistical, the second is the systematic, and the last due to the integrated luminosity.
description: The kinematic variables
describe the $\ell$+jets, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$), and the dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels.
The measured cross sections are given per decay channel and for their combination.

The fiducial region in the $\ell$+jets decay channel is defined as:
- $\equiv$1$\rm{e}$($\mu$), $p_T$&gt;35(25)GeV&&|$\eta$|&lt;2.1
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;15GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;10GeV&&|$\eta$|&lt;2.5 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.4
- 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 $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$

The acceptance is measured in the $\ell$+jets channel as:
0.301$\pm$0.007(tot)

The fiducial region in the dilepton decay channel is defined as: 
- $\geq1\rm{e}$ or $\mu$ with $p_T$&gt;20GeV&&|$\eta$|&lt;2.4 and $p_T$&gt;18GeV&&|$\eta$|&lt;2.1, respectively
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region for electrons
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;3.0
- min($\Delta R(jet,\ell)$) &gt; 0.3
- $M_{\ell \ell}$ &gt; 20 GeV
- 76 &lt;$M_{\ell \ell}$ &lt; 106 GeV and $p_{\rm{T}}^{\rm{mss}}$&gt;35 GeV only in the $\mu^\pm \mu^\mp$ channel
- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum

The acceptance is measured in the dilepton channel as:
0.53$\pm$0.01(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.37$\pm$0.01(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

The efficiency is measured in the dilepton channel as:
0.55$\pm$0.02(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.57$\pm$0.04(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

In both the $\ell$+jets and dilepton analyses, events with $\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.
DOI: 10.17182/hepdata.81690.v1/t3
title: "Table 3" of "Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton"

description: The measured total cross section in the combined $\ell$+jets and dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels. The weights of the individual measurements are 81.8% for $\ell$+jets, 13.5% for $\rm{e}^\pm \mu^\mp$, and 4.7% for $\mu^\pm \mu^\mp$ channels. The first uncertainty is the statistical, the second is the systematic, and the last due to the integrated luminosity.
description: The kinematic variables
describe the $\ell$+jets, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$), and the dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels.
The measured cross sections are given per decay channel and for their combination.

The fiducial region in the $\ell$+jets decay channel is defined as:
- $\equiv$1$\rm{e}$($\mu$), $p_T$&gt;35(25)GeV&&|$\eta$|&lt;2.1
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;15GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;10GeV&&|$\eta$|&lt;2.5 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.4
- 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 $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$

The acceptance is measured in the $\ell$+jets channel as:
0.301$\pm$0.007(tot)

The fiducial region in the dilepton decay channel is defined as: 
- $\geq1\rm{e}$ or $\mu$ with $p_T$&gt;20GeV&&|$\eta$|&lt;2.4 and $p_T$&gt;18GeV&&|$\eta$|&lt;2.1, respectively
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region for electrons
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;3.0
- min($\Delta R(jet,\ell)$) &gt; 0.3
- $M_{\ell \ell}$ &gt; 20 GeV
- 76 &lt;$M_{\ell \ell}$ &lt; 106 GeV and $p_{\rm{T}}^{\rm{mss}}$&gt;35 GeV only in the $\mu^\pm \mu^\mp$ channel
- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum

The acceptance is measured in the dilepton channel as:
0.53$\pm$0.01(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.37$\pm$0.01(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

The efficiency is measured in the dilepton channel as:
0.55$\pm$0.02(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.57$\pm$0.04(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

In both the $\ell$+jets and dilepton analyses, events with $\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.
DOI: 10.17182/hepdata.81690.v1/t4
title: "Table 4" of "Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton"

description: The observed distribution of the dijet invariant mass in the $\ell$+jets decay channel in the 0 b tagged jet category. The vertical bars on the data points represent the statistical uncertainties. The integral in the $\rm{e}$($\mu$)+jets channel (including overflow events) is 1375 (2406).
description: The kinematic variables
describe the $\ell$+jets, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$), and the dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels.
The measured cross sections are given per decay channel and for their combination.

The fiducial region in the $\ell$+jets decay channel is defined as:
- $\equiv$1$\rm{e}$($\mu$), $p_T$&gt;35(25)GeV&&|$\eta$|&lt;2.1
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;15GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;10GeV&&|$\eta$|&lt;2.5 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.4
- 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 $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$

The acceptance is measured in the $\ell$+jets channel as:
0.301$\pm$0.007(tot)

The fiducial region in the dilepton decay channel is defined as: 
- $\geq1\rm{e}$ or $\mu$ with $p_T$&gt;20GeV&&|$\eta$|&lt;2.4 and $p_T$&gt;18GeV&&|$\eta$|&lt;2.1, respectively
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region for electrons
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;3.0
- min($\Delta R(jet,\ell)$) &gt; 0.3
- $M_{\ell \ell}$ &gt; 20 GeV
- 76 &lt;$M_{\ell \ell}$ &lt; 106 GeV and $p_{\rm{T}}^{\rm{mss}}$&gt;35 GeV only in the $\mu^\pm \mu^\mp$ channel
- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum

The acceptance is measured in the dilepton channel as:
0.53$\pm$0.01(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.37$\pm$0.01(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

The efficiency is measured in the dilepton channel as:
0.55$\pm$0.02(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.57$\pm$0.04(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

In both the $\ell$+jets and dilepton analyses, events with $\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.
DOI: 10.17182/hepdata.81690.v1/t10
title: "Table 10" of "Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton"

description: The observed distribution of the jet multiplicity in the $\rm{e}^\pm \mu^\mp$ decay channel for events passing the dilepton criteria. The error bars indicate the statistical uncertainties. The last bin of the distributions contains the overflow events.
description: The kinematic variables
describe the $\ell$+jets, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$), and the dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels.
The measured cross sections are given per decay channel and for their combination.

The fiducial region in the $\ell$+jets decay channel is defined as:
- $\equiv$1$\rm{e}$($\mu$), $p_T$&gt;35(25)GeV&&|$\eta$|&lt;2.1
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;15GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;10GeV&&|$\eta$|&lt;2.5 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.4
- 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 $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$

The acceptance is measured in the $\ell$+jets channel as:
0.301$\pm$0.007(tot)

The fiducial region in the dilepton decay channel is defined as: 
- $\geq1\rm{e}$ or $\mu$ with $p_T$&gt;20GeV&&|$\eta$|&lt;2.4 and $p_T$&gt;18GeV&&|$\eta$|&lt;2.1, respectively
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region for electrons
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;3.0
- min($\Delta R(jet,\ell)$) &gt; 0.3
- $M_{\ell \ell}$ &gt; 20 GeV
- 76 &lt;$M_{\ell \ell}$ &lt; 106 GeV and $p_{\rm{T}}^{\rm{mss}}$&gt;35 GeV only in the $\mu^\pm \mu^\mp$ channel
- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum

The acceptance is measured in the dilepton channel as:
0.53$\pm$0.01(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.37$\pm$0.01(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

The efficiency is measured in the dilepton channel as:
0.55$\pm$0.02(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.57$\pm$0.04(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

In both the $\ell$+jets and dilepton analyses, events with $\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.
DOI: 10.17182/hepdata.81690.v1/t11
title: "Table 11" of "Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton"

description: The observed distribution of the scalar $p_{\rm{T}}$ sum of all jets in the $\rm{e}^\pm \mu^\mp$ decay channel for events passing the dilepton criteria. The error bars indicate the statistical uncertainties. The last bin of the distributions contains the overflow events.
description: The kinematic variables
describe the $\ell$+jets, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$), and the dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels.
The measured cross sections are given per decay channel and for their combination.

The fiducial region in the $\ell$+jets decay channel is defined as:
- $\equiv$1$\rm{e}$($\mu$), $p_T$&gt;35(25)GeV&&|$\eta$|&lt;2.1
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;15GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;10GeV&&|$\eta$|&lt;2.5 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.4
- 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 $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$

The acceptance is measured in the $\ell$+jets channel as:
0.301$\pm$0.007(tot)

The fiducial region in the dilepton decay channel is defined as: 
- $\geq1\rm{e}$ or $\mu$ with $p_T$&gt;20GeV&&|$\eta$|&lt;2.4 and $p_T$&gt;18GeV&&|$\eta$|&lt;2.1, respectively
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region for electrons
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;3.0
- min($\Delta R(jet,\ell)$) &gt; 0.3
- $M_{\ell \ell}$ &gt; 20 GeV
- 76 &lt;$M_{\ell \ell}$ &lt; 106 GeV and $p_{\rm{T}}^{\rm{mss}}$&gt;35 GeV only in the $\mu^\pm \mu^\mp$ channel
- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum

The acceptance is measured in the dilepton channel as:
0.53$\pm$0.01(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.37$\pm$0.01(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

The efficiency is measured in the dilepton channel as:
0.55$\pm$0.02(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.57$\pm$0.04(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

In both the $\ell$+jets and dilepton analyses, events with $\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.
DOI: 10.17182/hepdata.81690.v1/t12
title: "Table 12" of "Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton"

description: The observed distribution of the invariant mass of the lepton pair in the $\rm{e}^\pm \mu^\mp$ decay channel after requiring at least two jets. The error bars indicate the statistical uncertainties. The integral is 24. The last bin of the distributions contains the overflow events.
description: The kinematic variables
describe the $\ell$+jets, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$), and the dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels.
The measured cross sections are given per decay channel and for their combination.

The fiducial region in the $\ell$+jets decay channel is defined as:
- $\equiv$1$\rm{e}$($\mu$), $p_T$&gt;35(25)GeV&&|$\eta$|&lt;2.1
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;15GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;10GeV&&|$\eta$|&lt;2.5 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.4
- 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 $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$

The acceptance is measured in the $\ell$+jets channel as:
0.301$\pm$0.007(tot)

The fiducial region in the dilepton decay channel is defined as: 
- $\geq1\rm{e}$ or $\mu$ with $p_T$&gt;20GeV&&|$\eta$|&lt;2.4 and $p_T$&gt;18GeV&&|$\eta$|&lt;2.1, respectively
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region for electrons
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;3.0
- min($\Delta R(jet,\ell)$) &gt; 0.3
- $M_{\ell \ell}$ &gt; 20 GeV
- 76 &lt;$M_{\ell \ell}$ &lt; 106 GeV and $p_{\rm{T}}^{\rm{mss}}$&gt;35 GeV only in the $\mu^\pm \mu^\mp$ channel
- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum

The acceptance is measured in the dilepton channel as:
0.53$\pm$0.01(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.37$\pm$0.01(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

The efficiency is measured in the dilepton channel as:
0.55$\pm$0.02(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.57$\pm$0.04(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

In both the $\ell$+jets and dilepton analyses, events with $\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.
DOI: 10.17182/hepdata.81690.v1/t13
title: "Table 13" of "Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton"

description: The observed distribution of the $p_{\rm{T}}$ of the lepton pair in the $\rm{e}^\pm \mu^\mp$ decay channel after requiring at least two jets. The error bars indicate the statistical uncertainties. The integral is 24. The last bin of the distributions contains the overflow events.
description: The kinematic variables
describe the $\ell$+jets, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$), and the dilepton ($\rm{e}^\pm \mu^\mp$ or $\mu^\pm \mu^\mp$) decay channels.
The measured cross sections are given per decay channel and for their combination.

The fiducial region in the $\ell$+jets decay channel is defined as:
- $\equiv$1$\rm{e}$($\mu$), $p_T$&gt;35(25)GeV&&|$\eta$|&lt;2.1
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;15GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;10GeV&&|$\eta$|&lt;2.5 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.4
- 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 $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$

The acceptance is measured in the $\ell$+jets channel as:
0.301$\pm$0.007(tot)

The fiducial region in the dilepton decay channel is defined as: 
- $\geq1\rm{e}$ or $\mu$ with $p_T$&gt;20GeV&&|$\eta$|&lt;2.4 and $p_T$&gt;18GeV&&|$\eta$|&lt;2.1, respectively
- including the transition 1.444&lt;|$\eta$|&lt;1.566 region for electrons
- $\geq$2jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;3.0
- min($\Delta R(jet,\ell)$) &gt; 0.3
- $M_{\ell \ell}$ &gt; 20 GeV
- 76 &lt;$M_{\ell \ell}$ &lt; 106 GeV and $p_{\rm{T}}^{\rm{mss}}$&gt;35 GeV only in the $\mu^\pm \mu^\mp$ channel
- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum

The acceptance is measured in the dilepton channel as:
0.53$\pm$0.01(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.37$\pm$0.01(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

The efficiency is measured in the dilepton channel as:
0.55$\pm$0.02(tot) in the $\rm{e}^\pm \mu^\mp$ and 0.57$\pm$0.04(tot) in the $\mu^\pm \mu^\mp$ channel, respectively

In both the $\ell$+jets and dilepton analyses, events with $\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.