cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95826.v1/t84
title: "mllbb for b-associated production, 2 tag, mA 760 mH 640" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (760, 640) GeV in the 2 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (760, 640) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t85
title: "mllbb for b-associated production, 2 tag, mA 760 mH 650" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (760, 650) GeV in the 2 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (760, 650) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t86
title: "mllbb for b-associated production, 2 tag, mA 770 mH 660" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (770, 660) GeV in the 2 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (770, 660) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t87
title: "mllbb for b-associated production, 2 tag, mA 780 mH 670" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (780, 670) GeV in the 2 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (780, 670) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t88
title: "mllbb for b-associated production, 2 tag, mA 780 mH 680" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (780, 680) GeV in the 2 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (780, 680) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.3535/dm0-11w-wb3
title: Salix aurita L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95826.v1/t89
title: "mllbb for b-associated production, 2 tag, mA 790 mH 690" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (790, 690) GeV in the 2 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (790, 690) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t90
title: "mllbb for b-associated production, 3 tag, mA 440 mH 130" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (440, 130) GeV in the 3 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (440, 130) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t91
title: "mllbb for b-associated production, 3 tag, mA 450 mH 140" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (450, 140) GeV in the 3 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (450, 140) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t92
title: "mllbb for b-associated production, 3 tag, mA 460 mH 150" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (460, 150) GeV in the 3 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (460, 150) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t93
title: "mllbb for b-associated production, 3 tag, mA 460 mH 160" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (460, 160) GeV in the 3 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (460, 160) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t94
title: "mllbb for b-associated production, 3 tag, mA 470 mH 170" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (470, 170) GeV in the 3 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (470, 170) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t95
title: "mllbb for b-associated production, 3 tag, mA 470 mH 180" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (470, 180) GeV in the 3 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (470, 180) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t96
title: "mllbb for b-associated production, 3 tag, mA 420 mH 190" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mllbb mass distribution for the mbb window defined for (mA, mH) = (420, 190) GeV in the 3 tag category with b-associated production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (420, 190) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;bb) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.3535/0qh-zqp-q64
title: Acer campestre L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/t5y-epm-k76
title: Brachypodium sylvaticum (Huds.) P.Beauv.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95758.v1/t630
title: "Table 629" of "Measurements of top-quark pair differential and double-differential cross-sections in the $\ell$+jets channel with $pp$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector"

description: Relative differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
description: Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\bar{t}$ system and jet multiplicities. The study was performed using data from pp collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of 36 fb$^{−1}$. Due to the large $t\bar{t}$ cross-section at the LHC, such measurements allow a detailed study of the properties of top-quark production and decay, enabling precision tests of several Monte Carlo generators and fixed-order Standard Model predictions. Overall, there is good agreement between the theoretical predictions and the data.
DOI: 10.17182/hepdata.95758.v1/t634
title: "Table 633" of "Measurements of top-quark pair differential and double-differential cross-sections in the $\ell$+jets channel with $pp$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector"

description: Relative differential cross-section as a function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
description: Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\bar{t}$ system and jet multiplicities. The study was performed using data from pp collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of 36 fb$^{−1}$. Due to the large $t\bar{t}$ cross-section at the LHC, such measurements allow a detailed study of the properties of top-quark production and decay, enabling precision tests of several Monte Carlo generators and fixed-order Standard Model predictions. Overall, there is good agreement between the theoretical predictions and the data.
DOI: 10.17182/hepdata.95758.v1/t637
title: "Table 636" of "Measurements of top-quark pair differential and double-differential cross-sections in the $\ell$+jets channel with $pp$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector"

description: Covariance matrix of the Absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
description: Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\bar{t}$ system and jet multiplicities. The study was performed using data from pp collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of 36 fb$^{−1}$. Due to the large $t\bar{t}$ cross-section at the LHC, such measurements allow a detailed study of the properties of top-quark production and decay, enabling precision tests of several Monte Carlo generators and fixed-order Standard Model predictions. Overall, there is good agreement between the theoretical predictions and the data.