cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79162.v2/t1
title: "Figure 1a" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Signal acceptance times efficiency as a function of mass for Scalar → WW in the heavy scalar model
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t2
title: "Figure 1b" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Signal acceptance times efficiency as a function of mass for Z' → WW in the HVT model
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t3
title: "Figure 1c" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Signal acceptance times efficiency as a function of mass for GKK → WW in the bulk RS model
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t4
title: "Figure 4a" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Dijet mass distributions for data in the (a) WW signal region.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t5
title: "Figure 4b" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Dijet mass distributions for data in the (b) WZ signal region.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t6
title: "Figure 4c" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Dijet mass distributions for data in the (c) ZZ signal region.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t7
title: "Figure 4d" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Dijet mass distributions for data in the (d) WZ+WW signal region.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t8
title: "Figure 4e" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Dijet mass distributions for data in the (e) WW+ZZ signal region.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t10
title: "Figure 5b" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for WW+ZZ production as a function of GKK mass for the bulk RS model with k/M̄Pl=1.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t11
title: "Figure 5c" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for (c) WW+ZZ production as a function of scalar mass.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t12
title: "Figure Aux 2a" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for WW production as a function of V' mass
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t13
title: "Figure Aux 2b" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for WZ production as a function of V' mass
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t9
title: "Figure 5a" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for WW+WZ production as a function of V' mass
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t14
title: "Figure Aux 3a" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for WW production as a function of GKK mass for the bulk RS model with k/M̄Pl=0.5.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t15
title: "Figure Aux 3b" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for ZZ production as a function of GKK mass for the bulk RS model with k/M̄Pl=0.5.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t16
title: "Figure Aux 3c" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for WW production as a function of GKK mass for the bulk RS model with k/M̄Pl=1.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t17
title: "Figure Aux 3d" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for ZZ production as a function of GKK mass for the bulk RS model with k/M̄Pl=1.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t18
title: "Figure Aux 4" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for WW+ZZ production as a function of GKK mass for the bulk RS model with k/M̄Pl=0.5.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t19
title: "Figure Aux 5a" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for WW production as a function of scalar mass.
description: No data abstract available.
DOI: 10.17182/hepdata.79162.v2/t20
title: "Figure Aux 5b" of "Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits at the 95% CL on the cross section times branching ratio for ZZ production as a function of scalar mass.
description: No data abstract available.
DOI: 10.17182/hepdata.79163.v1/t1
title: "Table 1" of "Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector"

description: Measured fiducial integrated $\gamma+b$ and $\gamma+c$ cross sections for $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$.
description: This Letter presents the measurement of differential cross sections of isolated prompt photons produced in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The measurement uses proton--proton collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb$^{-1}$. The differential cross sections are measured for each jet flavour with respect to the transverse energy of the leading photon in two photon pseudorapidity regions: $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$. The measurement covers photon transverse energies $2525\text{ GeV}$
- $|\eta^\gamma|&lt;1.37$ or $1.56&lt;|\eta^\gamma|&lt;2.37$
- $E_\text{T}^\text{iso}&lt;4.8\text{ GeV}+0.0042\times E_\text{T}^\gamma$
- $p_\text{T}^\text{jet}&gt;20\text{ GeV}$
- $|y^\text{jet}|&lt;2.5$
- $\sqrt{(\Delta\phi)^2+(\Delta y)^2}&gt;1$
- The jet flavour is determined through hadron matching: at least one b-hadron satisfying $p_\text{T}^\text{hadron}&gt;5\text{ GeV}$ and $\Delta R &lt; 0.3$ between the hadron and the jet to label the jet as a b-jet or, if no b-hadrons satisfy these two cuts, at least one c-hadron satisfying the two cuts to label the jet as a c-jet.
DOI: 10.17182/hepdata.79163.v1/t2
title: "Table 2" of "Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector"

description: Measured $\gamma+b$ fiducial differential cross section as a function of $E_\text{T}^\gamma$ for $|\eta^\gamma|&lt;1.37$.
description: This Letter presents the measurement of differential cross sections of isolated prompt photons produced in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The measurement uses proton--proton collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb$^{-1}$. The differential cross sections are measured for each jet flavour with respect to the transverse energy of the leading photon in two photon pseudorapidity regions: $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$. The measurement covers photon transverse energies $2525\text{ GeV}$
- $|\eta^\gamma|&lt;1.37$ or $1.56&lt;|\eta^\gamma|&lt;2.37$
- $E_\text{T}^\text{iso}&lt;4.8\text{ GeV}+0.0042\times E_\text{T}^\gamma$
- $p_\text{T}^\text{jet}&gt;20\text{ GeV}$
- $|y^\text{jet}|&lt;2.5$
- $\sqrt{(\Delta\phi)^2+(\Delta y)^2}&gt;1$
- The jet flavour is determined through hadron matching: at least one b-hadron satisfying $p_\text{T}^\text{hadron}&gt;5\text{ GeV}$ and $\Delta R &lt; 0.3$ between the hadron and the jet to label the jet as a b-jet or, if no b-hadrons satisfy these two cuts, at least one c-hadron satisfying the two cuts to label the jet as a c-jet.
DOI: 10.17182/hepdata.79163.v1/t4
title: "Table 4" of "Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector"

description: Measured $\gamma+c$ fiducial differential cross section as a function of $E_\text{T}^\gamma$ for $|\eta^\gamma|&lt;1.37$.
description: This Letter presents the measurement of differential cross sections of isolated prompt photons produced in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The measurement uses proton--proton collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb$^{-1}$. The differential cross sections are measured for each jet flavour with respect to the transverse energy of the leading photon in two photon pseudorapidity regions: $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$. The measurement covers photon transverse energies $2525\text{ GeV}$
- $|\eta^\gamma|&lt;1.37$ or $1.56&lt;|\eta^\gamma|&lt;2.37$
- $E_\text{T}^\text{iso}&lt;4.8\text{ GeV}+0.0042\times E_\text{T}^\gamma$
- $p_\text{T}^\text{jet}&gt;20\text{ GeV}$
- $|y^\text{jet}|&lt;2.5$
- $\sqrt{(\Delta\phi)^2+(\Delta y)^2}&gt;1$
- The jet flavour is determined through hadron matching: at least one b-hadron satisfying $p_\text{T}^\text{hadron}&gt;5\text{ GeV}$ and $\Delta R &lt; 0.3$ between the hadron and the jet to label the jet as a b-jet or, if no b-hadrons satisfy these two cuts, at least one c-hadron satisfying the two cuts to label the jet as a c-jet.
DOI: 10.17182/hepdata.79163.v1/t3
title: "Table 3" of "Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector"

description: Measured $\gamma+b$ fiducial differential cross section as a function of $E_\text{T}^\gamma$ for $1.56&lt;|\eta^\gamma|&lt;2.37$.
description: This Letter presents the measurement of differential cross sections of isolated prompt photons produced in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The measurement uses proton--proton collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb$^{-1}$. The differential cross sections are measured for each jet flavour with respect to the transverse energy of the leading photon in two photon pseudorapidity regions: $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$. The measurement covers photon transverse energies $2525\text{ GeV}$
- $|\eta^\gamma|&lt;1.37$ or $1.56&lt;|\eta^\gamma|&lt;2.37$
- $E_\text{T}^\text{iso}&lt;4.8\text{ GeV}+0.0042\times E_\text{T}^\gamma$
- $p_\text{T}^\text{jet}&gt;20\text{ GeV}$
- $|y^\text{jet}|&lt;2.5$
- $\sqrt{(\Delta\phi)^2+(\Delta y)^2}&gt;1$
- The jet flavour is determined through hadron matching: at least one b-hadron satisfying $p_\text{T}^\text{hadron}&gt;5\text{ GeV}$ and $\Delta R &lt; 0.3$ between the hadron and the jet to label the jet as a b-jet or, if no b-hadrons satisfy these two cuts, at least one c-hadron satisfying the two cuts to label the jet as a c-jet.
DOI: 10.17182/hepdata.79163.v1/t5
title: "Table 5" of "Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector"

description: Measured $\gamma+c$ fiducial differential cross section as a function of $E_\text{T}^\gamma$ for $1.56&lt;|\eta^\gamma|&lt;2.37$.
description: This Letter presents the measurement of differential cross sections of isolated prompt photons produced in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The measurement uses proton--proton collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb$^{-1}$. The differential cross sections are measured for each jet flavour with respect to the transverse energy of the leading photon in two photon pseudorapidity regions: $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$. The measurement covers photon transverse energies $2525\text{ GeV}$
- $|\eta^\gamma|&lt;1.37$ or $1.56&lt;|\eta^\gamma|&lt;2.37$
- $E_\text{T}^\text{iso}&lt;4.8\text{ GeV}+0.0042\times E_\text{T}^\gamma$
- $p_\text{T}^\text{jet}&gt;20\text{ GeV}$
- $|y^\text{jet}|&lt;2.5$
- $\sqrt{(\Delta\phi)^2+(\Delta y)^2}&gt;1$
- The jet flavour is determined through hadron matching: at least one b-hadron satisfying $p_\text{T}^\text{hadron}&gt;5\text{ GeV}$ and $\Delta R &lt; 0.3$ between the hadron and the jet to label the jet as a b-jet or, if no b-hadrons satisfy these two cuts, at least one c-hadron satisfying the two cuts to label the jet as a c-jet.
DOI: 10.17182/hepdata.79163.v1/t6
title: "Table 6" of "Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector"

description: Measured ratio of the $\gamma+b$ fiducial differential cross section as a function of $E_\text{T}^\gamma$ for $|\eta^\gamma|&lt;1.37$ to that for $1.56&lt;|\eta^\gamma|&lt;2.37$.
description: This Letter presents the measurement of differential cross sections of isolated prompt photons produced in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The measurement uses proton--proton collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb$^{-1}$. The differential cross sections are measured for each jet flavour with respect to the transverse energy of the leading photon in two photon pseudorapidity regions: $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$. The measurement covers photon transverse energies $2525\text{ GeV}$
- $|\eta^\gamma|&lt;1.37$ or $1.56&lt;|\eta^\gamma|&lt;2.37$
- $E_\text{T}^\text{iso}&lt;4.8\text{ GeV}+0.0042\times E_\text{T}^\gamma$
- $p_\text{T}^\text{jet}&gt;20\text{ GeV}$
- $|y^\text{jet}|&lt;2.5$
- $\sqrt{(\Delta\phi)^2+(\Delta y)^2}&gt;1$
- The jet flavour is determined through hadron matching: at least one b-hadron satisfying $p_\text{T}^\text{hadron}&gt;5\text{ GeV}$ and $\Delta R &lt; 0.3$ between the hadron and the jet to label the jet as a b-jet or, if no b-hadrons satisfy these two cuts, at least one c-hadron satisfying the two cuts to label the jet as a c-jet.
DOI: 10.17182/hepdata.79163.v1/t7
title: "Table 7" of "Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector"

description: Measured ratio of the $\gamma+c$ fiducial differential cross section as a function of $E_\text{T}^\gamma$ for $|\eta^\gamma|&lt;1.37$ to that for $1.56&lt;|\eta^\gamma|&lt;2.37$.
description: This Letter presents the measurement of differential cross sections of isolated prompt photons produced in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The measurement uses proton--proton collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb$^{-1}$. The differential cross sections are measured for each jet flavour with respect to the transverse energy of the leading photon in two photon pseudorapidity regions: $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$. The measurement covers photon transverse energies $2525\text{ GeV}$
- $|\eta^\gamma|&lt;1.37$ or $1.56&lt;|\eta^\gamma|&lt;2.37$
- $E_\text{T}^\text{iso}&lt;4.8\text{ GeV}+0.0042\times E_\text{T}^\gamma$
- $p_\text{T}^\text{jet}&gt;20\text{ GeV}$
- $|y^\text{jet}|&lt;2.5$
- $\sqrt{(\Delta\phi)^2+(\Delta y)^2}&gt;1$
- The jet flavour is determined through hadron matching: at least one b-hadron satisfying $p_\text{T}^\text{hadron}&gt;5\text{ GeV}$ and $\Delta R &lt; 0.3$ between the hadron and the jet to label the jet as a b-jet or, if no b-hadrons satisfy these two cuts, at least one c-hadron satisfying the two cuts to label the jet as a c-jet.
DOI: 10.17182/hepdata.79163.v1/t10
title: "Table 10" of "Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector"

description: Signed shifts of the individual systematic uncertainties on the $\gamma+b$ cross section for $1.56&lt;|\eta^\gamma|&lt;2.37$. The numbers after the name of the uncertainty source refer to the individual component in that uncertainty. Each bin of the MC statistical uncertainty is independent of any other bin. The first four components of the photon energy scale uncertainty are specific to this $|\eta^\gamma|$ region and are independent of the components in the other region. The region is indicated as part of their name to indicate the independence between the $|\eta^\gamma|$ regions. The uncertainties on the prompt photon modelling, non-perturbative QCD models and particle-level migration effects are only varied once and not up and down by their nature, but are symmetrised for the final results. Only uncertainties which have at least a 1% variation in at least one bin of the $\gamma+b$ and $\gamma+c$ cross section measurements, including the ratios, are listed. The others are summed in quadrature and listed as a single entry.
description: This Letter presents the measurement of differential cross sections of isolated prompt photons produced in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The measurement uses proton--proton collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb$^{-1}$. The differential cross sections are measured for each jet flavour with respect to the transverse energy of the leading photon in two photon pseudorapidity regions: $|\eta^\gamma|&lt;1.37$ and $1.56&lt;|\eta^\gamma|&lt;2.37$. The measurement covers photon transverse energies $2525\text{ GeV}$
- $|\eta^\gamma|&lt;1.37$ or $1.56&lt;|\eta^\gamma|&lt;2.37$
- $E_\text{T}^\text{iso}&lt;4.8\text{ GeV}+0.0042\times E_\text{T}^\gamma$
- $p_\text{T}^\text{jet}&gt;20\text{ GeV}$
- $|y^\text{jet}|&lt;2.5$
- $\sqrt{(\Delta\phi)^2+(\Delta y)^2}&gt;1$
- The jet flavour is determined through hadron matching: at least one b-hadron satisfying $p_\text{T}^\text{hadron}&gt;5\text{ GeV}$ and $\Delta R &lt; 0.3$ between the hadron and the jet to label the jet as a b-jet or, if no b-hadrons satisfy these two cuts, at least one c-hadron satisfying the two cuts to label the jet as a c-jet.