cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.69247.v1/t7
title: "Table 7" of "$Z$ boson production in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV measured with the ATLAS detector"

description: The rapidity differential Z boson yields per event scaled by $\langle N_{coll}\rangle$ for three centrality ranges.
description: The ATLAS Collaboration has measured the inclusive production of $Z$ bosons via their decays into electron and muon pairs in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV at the Large Hadron Collider. The measurements are made using data corresponding to integrated luminosities of 29.4 nb$^{-1}$ and 28.1 nb$^{-1}$ for $Z \rightarrow ee$ and $Z \rightarrow \mu\mu$, respectively. The results from the two channels are consistent and combined to obtain a cross section times the $Z \rightarrow \ell\ell$ branching ratio, integrated over the rapidity region $|y^{*}_{Z}|&lt;3.5$, of 139.8 $\pm$ 4.8 (stat.) $\pm$ 6.2 (syst.) $\pm$ 3.8 (lumi.) nb. Differential cross sections are presented as functions of the $Z$ boson rapidity and transverse momentum, and compared with models based on parton distributions both with and without nuclear corrections. The centrality dependence of $Z$ boson production in $p+$Pb collisions is measured and analyzed within the framework of a standard Glauber model and the model's extension for fluctuations of the underlying nucleon-nucleon scattering cross section.
DOI: 10.17182/hepdata.69285.v1/t1
title: "Table 1" of "Angular coefficients of Z bosons produced in pp collisions at $\sqrt{s}$ = 8 TeV and decaying to $\mu^+ \mu^-$ as a function of transverse momentum and rapidity"

description: The five angular coefficients A0 to A4 and A0-A2 in bins of qT for |y| &lt; 1.
description: CERN-LHC. Measurements of the five most significant angular coefficients, A0 through A4, for Z bosons produced in pp collisions at sqrt(s) = 8 TeV and decaying to mu+mu- are presented as a function of the transverse momentum and rapidity of the Z boson. The integrated luminosity of the dataset collected with the CMS detector at the LHC corresponds to 19.7 inverse femtobarns. These measurements provide comprehensive information about the Z boson production mechanisms, and are compared to the QCD predictions at leading order, next-to-leading order, and next-to-next-to-leading order in perturbation theory.

The values of angular coefficients (A0, A1, A2, A3, A4, and A0-A2) are reported in the tables. See Phys. Lett. B 750 (2015) 154 for more details.
DOI: 10.17182/hepdata.69285.v1/t2
title: "Table 2" of "Angular coefficients of Z bosons produced in pp collisions at $\sqrt{s}$ = 8 TeV and decaying to $\mu^+ \mu^-$ as a function of transverse momentum and rapidity"

description: The five angular coefficients A0 to A4 and A0-A2 in bins of qT for 1 &lt; |y| &lt; 2.1.
description: CERN-LHC. Measurements of the five most significant angular coefficients, A0 through A4, for Z bosons produced in pp collisions at sqrt(s) = 8 TeV and decaying to mu+mu- are presented as a function of the transverse momentum and rapidity of the Z boson. The integrated luminosity of the dataset collected with the CMS detector at the LHC corresponds to 19.7 inverse femtobarns. These measurements provide comprehensive information about the Z boson production mechanisms, and are compared to the QCD predictions at leading order, next-to-leading order, and next-to-next-to-leading order in perturbation theory.

The values of angular coefficients (A0, A1, A2, A3, A4, and A0-A2) are reported in the tables. See Phys. Lett. B 750 (2015) 154 for more details.
DOI: 10.17182/hepdata.69286.v1/t1
title: "Table 1" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Fiducial cross-section SIG for the exclusive e+ e- and mu+ mu- production.
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t2
title: "Table 2" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Ratios of the number of observed to the number of expected events based on the MC predictions (R) for the exclusive e+ e- and mu+ mu- production.
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t3
title: "Table 3" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Detector response matrix (PROB) for the acoplanarity variable (ACO) for e+ e- channel (empty bins are not reported).
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t4
title: "Table 4" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Detector response matrix (PROB) for the acoplanarity variable (ACO) for mu+ mu- channel (empty bins are not reported).
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t5
title: "Table 5" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Acoplanarity (ACO) distributions unfolded for detector resolution, and lepton pair trigger, reconstruction and identification efficiencies for e+ e- channel (empty bins are not reported).
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t6
title: "Table 6" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Acoplanarity (ACO) distributions unfolded for detector resolution, and lepton pair trigger, reconstruction and identification efficiencies for mu+ mu- channel (empty bins are not reported).
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t7
title: "Table 7" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: The lepton pair exclusive selection efficiency in the fiducial region for signal MC events as a function of M and Y for e+ e- channel.
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t10
title: "Table 10" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: The lepton pair exclusive selection efficiency in the fiducial region for single-dissociative MC events as a function of M and Y for mu+ mu- channel.
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t8
title: "Table 8" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: The lepton pair exclusive selection efficiency in the fiducial region for signal MC events as a function of M and Y for mu+ mu- channel.
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69286.v1/t9
title: "Table 9" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: The lepton pair exclusive selection efficiency in the fiducial region for single-dissociative MC events as a function of M and Y for e+ e- channel.
description: CERN-LHC. This Letter reports a measurement of the exclusive $\gamma\gamma\rightarrow \ell^+\ell^- (\ell=e,~\mu)$ cross-section in proton-proton collisions at a centre-of-mass energy of $7~\mathrm{TeV}$ by the ATLAS experiment at the LHC, based on an integrated luminosity of $4.6~\mathrm{fb}^{-1}$. For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be $\sigma_{\gamma\gamma\rightarrow e^+e^-}^{\mathrm{excl.}} = 0.428~\pm~0.035~(\mathrm{stat.})~\pm~0.018~(\mathrm{syst.})~\mathrm{pb}$ for a phase-space region with invariant mass of the electron pairs greater than $24~\mathrm{GeV}$, in which both electrons have transverse momentum $p_\mathrm{T}&gt;12~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$. For muon pairs with invariant mass greater than $20~\mathrm{GeV}$, muons transverse momentum $p_\mathrm{T}&gt;10~\mathrm{GeV}$ and pseudorapidity $|\eta|&lt;2.4$, the cross-section is determined to be $\sigma_{\gamma\gamma\rightarrow \mu^+\mu^- }^{\mathrm{excl.}} = 0.628~\pm~0.032~(\mathrm{stat.}) ~\pm~0.021~(\mathrm{syst.})~\mathrm{pb}$. When proton absorptive effects due to finite proton size are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the prediction.
DOI: 10.17182/hepdata.69299.v1/t1
title: "Table 1" of "Search for Higgs boson pair production in the $b\bar{b} b\bar{b}$ final state from $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector"

description: 1D histogram of event yields as a function of reconstructed four-jet mass for the resolved analysis. The lower edge of the mass bin is given.
description: A search for Higgs boson pair production $pp\to hh$ is performed with 19.5 fb$^{-1}$ of proton--proton collision data at $\sqrt{s}=8$ TeV, which were recorded by the ATLAS detector at the Large Hadron Collider in 2012. The decay products of each Higgs boson are reconstructed as a high-momentum $b\bar{b}$ system with either a pair of small-radius jets or a single large-radius jet, the latter exploiting jet substructure techniques and associated $b$-tagged track-jets.
DOI: 10.17182/hepdata.69299.v1/t2
title: "Table 2" of "Search for Higgs boson pair production in the $b\bar{b} b\bar{b}$ final state from $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector"

description: 1D histogram of event yields as a function of reconstructed two-jet mass for the boosted analysis. The lower edge of the mass bin is given.
description: A search for Higgs boson pair production $pp\to hh$ is performed with 19.5 fb$^{-1}$ of proton--proton collision data at $\sqrt{s}=8$ TeV, which were recorded by the ATLAS detector at the Large Hadron Collider in 2012. The decay products of each Higgs boson are reconstructed as a high-momentum $b\bar{b}$ system with either a pair of small-radius jets or a single large-radius jet, the latter exploiting jet substructure techniques and associated $b$-tagged track-jets.
DOI: 10.17182/hepdata.69299.v1/t3
title: "Table 3" of "Search for Higgs boson pair production in the $b\bar{b} b\bar{b}$ final state from $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector"

description: The observed 95\% C.L. limit for $pp\rightarrow G^{*}_{KK}\rightarrow hh\rightarrow b\bar{b}b\bar{b}$ in the bulk RS model with $k/\bar{M}_{Pl} = 1$, as a function of resonance mass.
description: A search for Higgs boson pair production $pp\to hh$ is performed with 19.5 fb$^{-1}$ of proton--proton collision data at $\sqrt{s}=8$ TeV, which were recorded by the ATLAS detector at the Large Hadron Collider in 2012. The decay products of each Higgs boson are reconstructed as a high-momentum $b\bar{b}$ system with either a pair of small-radius jets or a single large-radius jet, the latter exploiting jet substructure techniques and associated $b$-tagged track-jets.