cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83200.v2/t20
title: "Table 20" of "Measurement of nuclear modification factors of $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) mesons in PbPb collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 TeV"

description: Nuclear modification factor of the Y(2S) meson as a function of collision centrality. Global uncertainty combines the pp luminosity and number of minimum bias events in PbPb collisions. The PP Y(2S) global uncertainty consists of the statistical and systematic uncertainties of pp yield for Y(2S) state.
description: CERN-LHC. The cross sections for $\Upsilon(\mathrm{1S})$, $\Upsilon(\mathrm{2S})$, and $\Upsilon(\mathrm{3S})$ production in lead-lead (PbPb) and proton-proton (pp) collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV have been measured using the CMS detector at the LHC. The nuclear modification factors, $ {R_{\mathrm{AA}}} $, derived from the PbPb-to-pp ratio of yields for each state, are studied as functions of meson rapidity and transverse momentum, as well as PbPb collision centrality. The yields of all three states are found to be significantly suppressed, and compatible with a sequential ordering of the suppression, $ {R_{\mathrm{AA}}}( \Upsilon(\mathrm{1S}) ) &gt; {R_{\mathrm{AA}}}( \Upsilon(\mathrm{2S})) &gt; {R_{\mathrm{AA}}} (\Upsilon(\mathrm{3S}) )$ . The suppression of $ \Upsilon(\mathrm{1S})$ is larger than that seen at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 2.76 TeV, although the two are compatible within uncertainties. The upper limit on the ${R_{\mathrm{AA}}}$ of $ \Upsilon(\mathrm{3S})$ integrated over $ {p_{\mathrm{T}}} $ and rapidity and centrality is 0.096 at 95% confidence level, which is the strongest suppression observed for any hadron species in heavy ion collisions to date.
DOI: 10.17182/hepdata.83200.v2/t21
title: "Table 21" of "Measurement of nuclear modification factors of $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) mesons in PbPb collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 TeV"

description: Confidence intervals on the nuclear modification factors of the Y(3S) mesons as a function of collision centrality.
description: CERN-LHC. The cross sections for $\Upsilon(\mathrm{1S})$, $\Upsilon(\mathrm{2S})$, and $\Upsilon(\mathrm{3S})$ production in lead-lead (PbPb) and proton-proton (pp) collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV have been measured using the CMS detector at the LHC. The nuclear modification factors, $ {R_{\mathrm{AA}}} $, derived from the PbPb-to-pp ratio of yields for each state, are studied as functions of meson rapidity and transverse momentum, as well as PbPb collision centrality. The yields of all three states are found to be significantly suppressed, and compatible with a sequential ordering of the suppression, $ {R_{\mathrm{AA}}}( \Upsilon(\mathrm{1S}) ) &gt; {R_{\mathrm{AA}}}( \Upsilon(\mathrm{2S})) &gt; {R_{\mathrm{AA}}} (\Upsilon(\mathrm{3S}) )$ . The suppression of $ \Upsilon(\mathrm{1S})$ is larger than that seen at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 2.76 TeV, although the two are compatible within uncertainties. The upper limit on the ${R_{\mathrm{AA}}}$ of $ \Upsilon(\mathrm{3S})$ integrated over $ {p_{\mathrm{T}}} $ and rapidity and centrality is 0.096 at 95% confidence level, which is the strongest suppression observed for any hadron species in heavy ion collisions to date.
DOI: 10.17182/hepdata.83200.v2/t22
title: "Table 22" of "Measurement of nuclear modification factors of $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) mesons in PbPb collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 TeV"

description: Confidence intervals on the nuclear modification factors of the Y(2S) mesons as a function of collision centrality.
description: CERN-LHC. The cross sections for $\Upsilon(\mathrm{1S})$, $\Upsilon(\mathrm{2S})$, and $\Upsilon(\mathrm{3S})$ production in lead-lead (PbPb) and proton-proton (pp) collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV have been measured using the CMS detector at the LHC. The nuclear modification factors, $ {R_{\mathrm{AA}}} $, derived from the PbPb-to-pp ratio of yields for each state, are studied as functions of meson rapidity and transverse momentum, as well as PbPb collision centrality. The yields of all three states are found to be significantly suppressed, and compatible with a sequential ordering of the suppression, $ {R_{\mathrm{AA}}}( \Upsilon(\mathrm{1S}) ) &gt; {R_{\mathrm{AA}}}( \Upsilon(\mathrm{2S})) &gt; {R_{\mathrm{AA}}} (\Upsilon(\mathrm{3S}) )$ . The suppression of $ \Upsilon(\mathrm{1S})$ is larger than that seen at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 2.76 TeV, although the two are compatible within uncertainties. The upper limit on the ${R_{\mathrm{AA}}}$ of $ \Upsilon(\mathrm{3S})$ integrated over $ {p_{\mathrm{T}}} $ and rapidity and centrality is 0.096 at 95% confidence level, which is the strongest suppression observed for any hadron species in heavy ion collisions to date.
DOI: 10.17182/hepdata.83200.v2/t23
title: "Table 23" of "Measurement of nuclear modification factors of $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) mesons in PbPb collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 TeV"

description: Nuclear modification factors of the Y(1S) and Y(2S) mesons in the integrated pT, rapidity and centrality.
description: CERN-LHC. The cross sections for $\Upsilon(\mathrm{1S})$, $\Upsilon(\mathrm{2S})$, and $\Upsilon(\mathrm{3S})$ production in lead-lead (PbPb) and proton-proton (pp) collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV have been measured using the CMS detector at the LHC. The nuclear modification factors, $ {R_{\mathrm{AA}}} $, derived from the PbPb-to-pp ratio of yields for each state, are studied as functions of meson rapidity and transverse momentum, as well as PbPb collision centrality. The yields of all three states are found to be significantly suppressed, and compatible with a sequential ordering of the suppression, $ {R_{\mathrm{AA}}}( \Upsilon(\mathrm{1S}) ) &gt; {R_{\mathrm{AA}}}( \Upsilon(\mathrm{2S})) &gt; {R_{\mathrm{AA}}} (\Upsilon(\mathrm{3S}) )$ . The suppression of $ \Upsilon(\mathrm{1S})$ is larger than that seen at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 2.76 TeV, although the two are compatible within uncertainties. The upper limit on the ${R_{\mathrm{AA}}}$ of $ \Upsilon(\mathrm{3S})$ integrated over $ {p_{\mathrm{T}}} $ and rapidity and centrality is 0.096 at 95% confidence level, which is the strongest suppression observed for any hadron species in heavy ion collisions to date.
DOI: 10.17182/hepdata.83201.v1/t1
title: "Results" of "Inclusive search for a highly boosted Higgs boson decaying to a bottom quark-antiquark pair"

description: Fitted signal strength, expected and observed significance of the Higgs and Z boson signal. The 95% confidence level upper limit (UL) on the Higgs boson signal strength is also listed.
description: No data abstract available.
DOI: 10.17182/hepdata.83201.v1/t2
title: "$m_{SD}$ distribution, double-b tagger passing region" of "Inclusive search for a highly boosted Higgs boson decaying to a bottom quark-antiquark pair"

description: The $m_{SD}$ distributions in data for the failing (left) and passing (right) regions and combined $p_{T}$ categories. The QCD multijet background in the passing region is predicted using the failing region and the pass-fail ratio $R_{p/f}$. The features at 166 and 180 GeV in the $m_{SD}$ distribution are due to the kinematic selection on $\rho$, which affects each $p_{T}$ category differently. In the bottom panel, the ratio of the data to its statistical uncertainty, after subtracting the nonresonant backgrounds, is shown.
description: No data abstract available.
DOI: 10.17182/hepdata.83201.v1/t3
title: "$m_{SD}$ distribution, double-b tagger failing region" of "Inclusive search for a highly boosted Higgs boson decaying to a bottom quark-antiquark pair"

description: The $m_{SD}$ distributions in data for the failing (left) and passing (right) regions and combined $p_{T}$ categories. The QCD multijet background in the passing region is predicted using the failing region and the pass-fail ratio $R_{p/f}$. The features at 166 and 180 GeV in the $m_{SD}$ distribution are due to the kinematic selection on $\rho$, which affects each $p_{T}$ category differently. In the bottom panel, the ratio of the data to its statistical uncertainty, after subtracting the nonresonant backgrounds, is shown.
description: No data abstract available.
DOI: 10.17182/hepdata.83201.v1/t4
title: "Profle likelihood scan $-2\Delta log L(\mu_{H}, \mu_{Z})$" of "Inclusive search for a highly boosted Higgs boson decaying to a bottom quark-antiquark pair"

description: Profile likelihood test statistic $-2\Delta log L$ scan in data as a function of the Higgs and Z bosons signal strengths $(\mu_{H}, \mu_{Z})$.
description: No data abstract available.
DOI: 10.17182/hepdata.83201.v1/t5
title: "68% CL contour on $(\mu_{H}, \mu_{Z})$" of "Inclusive search for a highly boosted Higgs boson decaying to a bottom quark-antiquark pair"

description: 68% CL contour as a function of the Higgs and Z bosons signal strengths $(\mu_{H}, \mu_{Z})$.
description: No data abstract available.
DOI: 10.17182/hepdata.83201.v1/t6
title: "95% CL contour on $(\mu_{H}, \mu_{Z})$" of "Inclusive search for a highly boosted Higgs boson decaying to a bottom quark-antiquark pair"

description: 95\% CL contour as a function of the Higgs and Z bosons signal strengths $(\mu_{H}, \mu_{Z})$.
description: No data abstract available.
DOI: 10.17182/hepdata.83202.v1/t1
title: "Table 1" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Differential cross sections in the full phase space obtained from the H-&gt;gammagamma and H-&gt;4l combined measurement for Higgs boson transverse momentum ptH. The NNLOPS ggF prediction scaled to the N3LO cross section is also provided.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t2
title: "Table 2" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Differential cross sections in the full phase space obtained from the H-&gt;gammagamma and H-&gt;4l combined measurement for the Higgs boson rapidity |yH|. The NNLOPS ggF prediction scaled to the N3LO cross section is also provided.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t3
title: "Table 3" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Differential cross sections in the full phase space obtained from the H-&gt;gammagamma and H-&gt;4l combined measurement for the number of jets Njets with pT &gt; 30 GeV. The NNLOPS ggF prediction scaled to the N3LO cross section is also provided.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t4
title: "Table 4" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Differential cross sections in the full phase space obtained from the H-&gt;gammagamma and H-&gt;4l combined measurement for the transverse momentum of the leading jet pTj1. The first bin in the pTj1 distribution corresponds to the 0-jet bin in the Njets distribution. The NNLOPS ggF prediction scaled to the N3LO cross section is also provided.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t5
title: "Table 5" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance factors to extrapolate from the fiducial phase space to the total phase space, in bins of Higgs transverse momentum, in the 4l channel.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t6
title: "Table 6" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance factors to extrapolate from the fiducial phase space to the total phase space, in bins of Higgs transverse momentum, in the gamma gamma channel.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t7
title: "Table 7" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance factors to extrapolate from the fiducial phase space to the total phase space, in bins of Higgs rapidity, in the 4l channel.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t10
title: "Table 10" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance factors to extrapolate from the fiducial phase space to the total phase space, in bins of number of jets, in the gamma gamma channel.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t11
title: "Table 11" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance factors to extrapolate from the fiducial phase space to the total phase space, in bins of the transverse momentum of the leading jet, in the 4l channel.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t12
title: "Table 12" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance factors to extrapolate from the fiducial phase space to the total phase space, in bins of the transverse momentum of the leading jet, in the gamma gamma channel.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t8
title: "Table 8" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance factors to extrapolate from the fiducial phase space to the total phase space, in bins of Higgs rapidity, in the gamma gamma channel.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83202.v1/t9
title: "Table 9" of "Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance factors to extrapolate from the fiducial phase space to the total phase space, in bins of number of jets, in the 4l channel.
description: CERN-LHC. Combined measurement of Higgs boson differential cross sections using 36.1 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are diphoton and four-lepton. The definition of fiducial region can be found in JHEP 03 (2018) 095 for the four-lepton decay channel, and arXiv:1802.04146 (submitted to PRD) for the diphoton decay channel. The measurements in the fiducial regions are extrapolated to the full phase-space before they are combined between the two channels.
DOI: 10.17182/hepdata.83203.v1/t1
title: "Figure 8: 95% CL upper limit on XSEC times BR" of "Search for charged Higgs bosons decaying into top and bottom quarks at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed limits for the production of $H^{+} \to tb$ in association with a top quark and a bottom quark. The bands surrounding the expected limit show the 68% and 95% confidence intervals. The limits are based on the combination of the $\ell+$jets and $\ell\ell$ final states. Theory predictions are shown for three representative values of $\tan\beta$ in the $m_h^{\mathrm{mod-}}$ benchmark scenario. Uncertainties in the predicted $H^+$ cross-sections or branching ratios are not considered.
description: CERN-LHC. A search for charged Higgs bosons heavier than the top quark and decaying via $H^\pm\to tb$ is presented. The dataset analysed corresponds to 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=13$ TeV and was recorded with the ATLAS detector at the LHC in 2015 and 2016. The production of a charged Higgs boson in association with a top quark and a bottom quark, $pp \to tbH^\pm$, is explored in the mass range from $m_{H^\pm}=200$ to $2000$ GeV using multi-jet final states with one or two electrons or muons. Events are categorised according to the multiplicity of jets and how likely these are to have originated from hadronisation of a bottom quark. Multivariate techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and exclusion limits are derived for the production cross-section times branching ratio of a charged Higgs boson as a function of its mass, which range from 2.9 pb at $m_{H^\pm} = 200$ GeV to 0.070 pb at $m_{H^\pm} = 2000$ GeV. The results are interpreted in two benchmark scenarios of the Minimal Supersymmetric Standard Model.