cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.81708.v1/t3
title: "Table 3" 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(a--&gt;mumu)*B(a--&gt;bb) assuming SM h production rates for pseudoscalar mass points between 25 and 62.5 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/t4
title: "Table 4" 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(a--&gt;mumu)*B(a--&gt;bb) assuming SM h production rates for pseudoscalar mass points between 25 and 62.5 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/t5
title: "Table 5" 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(a--&gt;mumu)*B(a--&gt;tautau) assuming SM h production rates for pseudoscalar mass points between 15 and 62.5 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/t6
title: "Table 6" 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(a--&gt;mumu)*B(a--&gt;tautau) assuming SM h production rates for pseudoscalar mass points between 15 and 62.5 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.81709.v1/t1
title: "Table 0" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: inclusive absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t2
title: "Table 1" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: $p_{T}^{t,1}$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t3
title: "Table 2" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: ${y}^{t,1}$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t4
title: "Table 3" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: $p_{T}^{t,2}$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t5
title: "Table 4" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: ${y}^{t,2}$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t6
title: "Table 5" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: $m^{t\bar{t}}$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t7
title: "Table 6" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: $p_{T}^{t\bar{t}}$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t8
title: "Table 7" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: $|y^{t\bar{t}}|$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t9
title: "Table 8" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: $\chi^{t\bar{t}}$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.
DOI: 10.17182/hepdata.81709.v1/t10
title: "Table 9" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector"

description: $y_{B}^{t\bar{t}}$ absolute differential cross-section in particle level
description: Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and $t\bar{t}$ system kinematic observables using proton--proton collisions at a center-of-mass energy of $\sqrt{s} = 13$ TeV. The data set corresponds to an integrated luminosity of $36.1$ fb$^{-1}$, recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Events with two large-radius jets in the final state, one with transverse momentum $p_{\rm T} &gt; 500$ GeV and a second with $p_{\rm T} &gt; 350$ GeV, are used for the measurement. The top-quark candidates are separated from the multijet background using jet substructure information and association with a $b$-tagged jet. The measured spectra are corrected for detector effects to a particle-level fiducial phase space and a parton-level limited phase space, and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ values. The cross-section for $t\bar{t}$ production in the fiducial phase-space region is $292 \pm 7 \rm{(stat)} \pm 76 \rm{(syst)}$ fb, to be compared to the theoretical prediction of $384 \pm 36$ fb.