cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.81690.v1/t5
title: "Table 5" 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 1 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 61 (129).
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/t6
title: "Table 6" 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 $\geq$2 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 19 (33).
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/t7
title: "Table 7" 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 the minimum angular distance $\Delta R$ between all pairs of jets $j$ and $j'$ 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/t8
title: "Table 8" 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 the minimum angular distance $\Delta R$ between all pairs of jets $j$ and $j'$ in the $\ell$+jets decay channel in the 1 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 61 (129).
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/t9
title: "Table 9" 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 the minimum angular distance $\Delta R$ between all pairs of jets $j$ and $j'$ in the $\ell$+jets decay channel in the $\geq$2 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 19 (33).
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/t14
title: "Table 14" 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 $p_{\rm{T}}^{\rm{miss}}$ in the $\mu^\pm \mu^\mp$ decay channel for events passing the dilepton criteria and Z boson veto. 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/t15
title: "Table 15" 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 $\mu^\pm \mu^\mp$ decay channel for events passing the dilepton criteria, Z boson veto, and $p_{\rm{T}}^{\rm{miss}}&gt;35$ GeV requirement. 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.81708.v1/t1
title: "Table 1" of "Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at sqrt(s) = 8 TeV"

description: Median expected 95% CL limits on the branching fraction B(h--&gt;aa)*B^2(a--&gt;tautau) assuming SM h production rates for pseudoscalar mass points between 5 and 15 GeV.
description: CERN-LHC. Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.7 fb^-1 of data collected in 2012. The final states used are 4 taus, 2 muons and 2 taus, and 2 muons and 2 b quarks.

The uncertainty on the global normalisation ("Lumi") remains at 2.6%. See http://cms-results.web.cern.ch/cms-results/public-results/preliminary-results/LUM-13-001/index.html for more details.

The 4tau channel fiducial region is defined as:
- 1st tau_mu, pT &gt; 25 GeV, |eta| &lt; 2.1
- 2nd tau_mu, pT &gt; 5 GeV, |eta| &lt; 2.1
- Tau_had, pT &gt; 20 GeV, |eta| &lt; 2.3
- DeltaR(1st tau_mu, 2nd tau_mu) &gt; 0.4
- DeltaR(1st tau_mu, tau_had) &gt; 0.5
- If &gt;1 pair of 2nd tau_mu and tau_had exists, the pair with higher tau_mu+tau_had visible mass is chosen
- Visible mass (2nd tau_mu, tau_had) &gt; 4 GeV

The 2mu2tau channel fiducial region is defined as:
- Any di-tau pair decay accepted except tau_mu+tau_mu
- ptMu1 &gt; 18 GeV, pTMu2 &gt; 9 GeV
- |etaMu| &lt; 2.4
- pTTauE &gt; 7 GeV, pTTauMu &gt; 5 GeV, pTTauHad &gt; 15 GeV
- |etaTauE| &lt; 2.5, |etaTauMu| &lt; 2.4, |etaTauHad| &lt; 2.3
- |Visible mass (mum, mu, tau, tau) - 125 GeV| &lt; 25 GeV
- DeltaR between all pairs of leptons &gt; 0.4
- No events with a b jet
- No events with &gt;4 leptons passing ID criteria
- (|m_mumu - m_tautau|/m_mumu) &lt; 0.8 (m_tautau is reconstructed with a maximum likelihood algorithm to correct for the neutrino momentum)

The 2mu2b channel fiducial region is defined as:
- ptMu1 &gt; 24 GeV, pTMu2 &gt; 9 GeV
- At least 2 b jets with pT &gt; 15 GeV and |eta| &lt; 2.4
- MET significance &lt; 6
- |m_mumubb - 125 GeV| &lt; 25 GeV
DOI: 10.17182/hepdata.81708.v1/t2
title: "Table 2" of "Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at sqrt(s) = 8 TeV"

description: Median observed 95% CL limits on the branching fraction B(h--&gt;aa)*B^2(a--&gt;tautau) assuming SM h production rates for pseudoscalar mass points between 5 and 15 GeV.
description: CERN-LHC. Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.7 fb^-1 of data collected in 2012. The final states used are 4 taus, 2 muons and 2 taus, and 2 muons and 2 b quarks.

The uncertainty on the global normalisation ("Lumi") remains at 2.6%. See http://cms-results.web.cern.ch/cms-results/public-results/preliminary-results/LUM-13-001/index.html for more details.

The 4tau channel fiducial region is defined as:
- 1st tau_mu, pT &gt; 25 GeV, |eta| &lt; 2.1
- 2nd tau_mu, pT &gt; 5 GeV, |eta| &lt; 2.1
- Tau_had, pT &gt; 20 GeV, |eta| &lt; 2.3
- DeltaR(1st tau_mu, 2nd tau_mu) &gt; 0.4
- DeltaR(1st tau_mu, tau_had) &gt; 0.5
- If &gt;1 pair of 2nd tau_mu and tau_had exists, the pair with higher tau_mu+tau_had visible mass is chosen
- Visible mass (2nd tau_mu, tau_had) &gt; 4 GeV

The 2mu2tau channel fiducial region is defined as:
- Any di-tau pair decay accepted except tau_mu+tau_mu
- ptMu1 &gt; 18 GeV, pTMu2 &gt; 9 GeV
- |etaMu| &lt; 2.4
- pTTauE &gt; 7 GeV, pTTauMu &gt; 5 GeV, pTTauHad &gt; 15 GeV
- |etaTauE| &lt; 2.5, |etaTauMu| &lt; 2.4, |etaTauHad| &lt; 2.3
- |Visible mass (mum, mu, tau, tau) - 125 GeV| &lt; 25 GeV
- DeltaR between all pairs of leptons &gt; 0.4
- No events with a b jet
- No events with &gt;4 leptons passing ID criteria
- (|m_mumu - m_tautau|/m_mumu) &lt; 0.8 (m_tautau is reconstructed with a maximum likelihood algorithm to correct for the neutrino momentum)

The 2mu2b channel fiducial region is defined as:
- ptMu1 &gt; 24 GeV, pTMu2 &gt; 9 GeV
- At least 2 b jets with pT &gt; 15 GeV and |eta| &lt; 2.4
- MET significance &lt; 6
- |m_mumubb - 125 GeV| &lt; 25 GeV