cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79924.v1/t11
title: "Table 11" of "Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Fiducial acceptance and product of the fiducial acceptance times the combined reconstruction and identification efficiency as a function of the mass for a spin-0 resonant signal with narrow width under the spin-0 selection. Only MC statistical uncertainties are included.
description: CERN-LHC. Search for new phenomena in high-mass diphoton final states using 37 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 2 photons.

The fiducial region for the spin-0 resonance search is defined as:
- 2 photons
- E_T &gt; 0.4 m_gamgam for the photon with leading E_T, and E_T &gt; 0.3 m_gamgam for the photon with sub-leading E_T
- |eta_gam| &lt; 2.37
- An isolation requirement using all particles with lifetime greater than 10 ps at the generator level in a cone of Delta_R = 0.4 around the photon direction: E^iso_T&lt; 0.05 E_T+ 6 GeV.

For the spin-2 resonance search, the acceptance and efficiencies are assumed to be those obtained from MC simulation of KK graviton decays.
DOI: 10.17182/hepdata.79924.v1/t12
title: "Table 12" of "Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Fiducial acceptance and product of the fiducial acceptance times the combined reconstruction and identification efficiency as a function of the mass for a spin-2 resonant signal with k/MPl=0.1 under the spin-2 selection. The definition of fiducial region is provided in JHEP 09 (2016) 001. Only MC statistical uncertainties are included.
description: CERN-LHC. Search for new phenomena in high-mass diphoton final states using 37 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 2 photons.

The fiducial region for the spin-0 resonance search is defined as:
- 2 photons
- E_T &gt; 0.4 m_gamgam for the photon with leading E_T, and E_T &gt; 0.3 m_gamgam for the photon with sub-leading E_T
- |eta_gam| &lt; 2.37
- An isolation requirement using all particles with lifetime greater than 10 ps at the generator level in a cone of Delta_R = 0.4 around the photon direction: E^iso_T&lt; 0.05 E_T+ 6 GeV.

For the spin-2 resonance search, the acceptance and efficiencies are assumed to be those obtained from MC simulation of KK graviton decays.
DOI: 10.17182/hepdata.79924.v1/t13
title: "Table 13" of "Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Fiducial acceptance and product of the fiducial acceptance times the combined reconstruction and identification efficiency as a function of the mass for an ADD excess (GRW formalism), calculated as the difference between the sum of ADD and SM contributions (including their interference) and the SM contribution, under the spin-2 selection in the signal region M(gamma gamma)&gt;2240 GeV. The definition of fiducial region is provided in JHEP 09 (2016) 001, and M(gamma gamma)&gt;2240 GeV is required in addition. Only MC statistical uncertainties are included.
description: CERN-LHC. Search for new phenomena in high-mass diphoton final states using 37 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 2 photons.

The fiducial region for the spin-0 resonance search is defined as:
- 2 photons
- E_T &gt; 0.4 m_gamgam for the photon with leading E_T, and E_T &gt; 0.3 m_gamgam for the photon with sub-leading E_T
- |eta_gam| &lt; 2.37
- An isolation requirement using all particles with lifetime greater than 10 ps at the generator level in a cone of Delta_R = 0.4 around the photon direction: E^iso_T&lt; 0.05 E_T+ 6 GeV.

For the spin-2 resonance search, the acceptance and efficiencies are assumed to be those obtained from MC simulation of KK graviton decays.
DOI: 10.17182/hepdata.79924.v1/t8
title: "Table 8" of "Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Upper limits on the production cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of the lightest KK graviton as a function of its mass m_G* for k/MPl=0.30.
description: CERN-LHC. Search for new phenomena in high-mass diphoton final states using 37 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 2 photons.

The fiducial region for the spin-0 resonance search is defined as:
- 2 photons
- E_T &gt; 0.4 m_gamgam for the photon with leading E_T, and E_T &gt; 0.3 m_gamgam for the photon with sub-leading E_T
- |eta_gam| &lt; 2.37
- An isolation requirement using all particles with lifetime greater than 10 ps at the generator level in a cone of Delta_R = 0.4 around the photon direction: E^iso_T&lt; 0.05 E_T+ 6 GeV.

For the spin-2 resonance search, the acceptance and efficiencies are assumed to be those obtained from MC simulation of KK graviton decays.
DOI: 10.17182/hepdata.79924.v1/t9
title: "Table 9" of "Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Distribution of the diphoton invariant mass for data events passing the spin-0 selection. The data points are plotted at the centre of each bin. The error bars indicate statistical uncertainties. The distribution consists of not only genuine diphoton events, but also events where at least one photon is faked by a jet. There is no data event above 2700 GeV.
description: CERN-LHC. Search for new phenomena in high-mass diphoton final states using 37 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 2 photons.

The fiducial region for the spin-0 resonance search is defined as:
- 2 photons
- E_T &gt; 0.4 m_gamgam for the photon with leading E_T, and E_T &gt; 0.3 m_gamgam for the photon with sub-leading E_T
- |eta_gam| &lt; 2.37
- An isolation requirement using all particles with lifetime greater than 10 ps at the generator level in a cone of Delta_R = 0.4 around the photon direction: E^iso_T&lt; 0.05 E_T+ 6 GeV.

For the spin-2 resonance search, the acceptance and efficiencies are assumed to be those obtained from MC simulation of KK graviton decays.
DOI: 10.17182/hepdata.79947.v1/t1
title: "Table 1" of "Measurement of the exclusive $\gamma \gamma \rightarrow \mu^+ \mu^-$ process in proton--proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The measured fiducial cross section.
description: CERN-LHC. Production of exclusive $pp \rightarrow pp \mu^+ \mu^-$ events at pp centre-of-mass energy of 13 TeV.
The fiducial region is defined as:
- exactly 2 muons
- $|\eta^{\mu}|$ &lt; 2.4
- 12 GeV &lt; $m_{\mu^+ \mu^-}$ &lt; 70 GeV
- $p_T^{\mu}$ &gt; 6 GeV, if 12 GeV &lt; $m_{\mu^+ \mu^-}$ &lt; 30 GeV
- $p_T^{\mu}$ &gt; 10 GeV, if 30 GeV &lt; $m_{\mu^+ \mu^-}$ &lt; 70 GeV
DOI: 10.17182/hepdata.79947.v1/t2
title: "Table 2" of "Measurement of the exclusive $\gamma \gamma \rightarrow \mu^+ \mu^-$ process in proton--proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Differential fiducial cross section in bins of the dimuon invariant mass. The measurements are listed together with the statistical and systematic uncertainties. The systematic uncertainties are separated into 2 uncorrelated, 7 correlated sources and the luminosity uncertainty. The sign of the uncertainty corresponds to a one standard deviation upward shift of the uncertainty source, where +/- means "+" and -/+ means "-".
description: CERN-LHC. Production of exclusive $pp \rightarrow pp \mu^+ \mu^-$ events at pp centre-of-mass energy of 13 TeV.
The fiducial region is defined as:
- exactly 2 muons
- $|\eta^{\mu}|$ &lt; 2.4
- 12 GeV &lt; $m_{\mu^+ \mu^-}$ &lt; 70 GeV
- $p_T^{\mu}$ &gt; 6 GeV, if 12 GeV &lt; $m_{\mu^+ \mu^-}$ &lt; 30 GeV
- $p_T^{\mu}$ &gt; 10 GeV, if 30 GeV &lt; $m_{\mu^+ \mu^-}$ &lt; 70 GeV
DOI: 10.17182/hepdata.79948.v1/t1
title: "Table 1" of "High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector"

description: Measured cross sections for isolated-photon plus 1jet production as a function of $E_{\rm T}^{\gamma}$.
description: CERN-LHC. Measurements of the cross section for prompt photon plus jet production in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.2/fb of data collected in 2012.

The photon is required to have a transverse energy above 130 GeV and absolute value of pseudorapity |etaGamma|&lt;2.37, excluding the region 1.37&lt;|etaGamma|&lt;1.56. The photon isolation is ensured by requiring the transverse energy around a cone of radius R=0.4 around the photon to be less than 10 GeV. At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons.

Jets are reconstructed using the anti-kt algorithm with radius parameter R=0.6 and required to have the jet rapidity in the range |yjet|&lt;4.4 and the distance between the jet and the photon DeltaR(gamma jet)&gt;1. The requirements on the jet transverse momenta depend on the sample and are as follows.

Photon+1jet sample (tables 1 and 2): pTjet1 &gt; 100 GeV.

Photon+1jet sample (tables 3 to 13): pTjet1 &gt; 100 GeV, |yjet1| &lt; 2.37, |costhetastar| &lt; 0.83 and |etaGamma + yjet1| &lt; 2.37 and mgammajet1 &gt; 467 GeV.

Photon+2jet sample (tables 14 to 17): pTjet1 &gt; 100 GeV and pTjet2 &gt; 65 GeV.

Photon+2jet sample (tables 18 and 20): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+2jet sample (tables 19 and 21): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and ETGamma &gt; 300 GeV.

Photon+2jet sample (table 22): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(jet1 jet2) &lt; 1.5 and |etajet1| &lt; 2.37.

Photon+2jet sample (table 23): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(gamma jet2) &lt; 1.5, |etajet1| &lt; 2.37 and pTjet2 &lt; ETGamma.

Photon+2jet sample (table 24): ratio of cross sections in tables 22 and 23.

Photon+3jet sample (tables 25 to 29): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and pTjet3 &gt; 50 GeV.

Photon+3jet sample (tables 30, 32 and 34): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+3jet sample (tables 31, 33 and 35): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and ETGamma &gt; 300 GeV.
DOI: 10.17182/hepdata.79948.v1/t2
title: "Table 2" of "High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector"

description: Measured cross sections for isolated-photon plus 1jet production as a function of $p_{\rm T}^{\rm jet1}$.
description: CERN-LHC. Measurements of the cross section for prompt photon plus jet production in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.2/fb of data collected in 2012.

The photon is required to have a transverse energy above 130 GeV and absolute value of pseudorapity |etaGamma|&lt;2.37, excluding the region 1.37&lt;|etaGamma|&lt;1.56. The photon isolation is ensured by requiring the transverse energy around a cone of radius R=0.4 around the photon to be less than 10 GeV. At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons.

Jets are reconstructed using the anti-kt algorithm with radius parameter R=0.6 and required to have the jet rapidity in the range |yjet|&lt;4.4 and the distance between the jet and the photon DeltaR(gamma jet)&gt;1. The requirements on the jet transverse momenta depend on the sample and are as follows.

Photon+1jet sample (tables 1 and 2): pTjet1 &gt; 100 GeV.

Photon+1jet sample (tables 3 to 13): pTjet1 &gt; 100 GeV, |yjet1| &lt; 2.37, |costhetastar| &lt; 0.83 and |etaGamma + yjet1| &lt; 2.37 and mgammajet1 &gt; 467 GeV.

Photon+2jet sample (tables 14 to 17): pTjet1 &gt; 100 GeV and pTjet2 &gt; 65 GeV.

Photon+2jet sample (tables 18 and 20): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+2jet sample (tables 19 and 21): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and ETGamma &gt; 300 GeV.

Photon+2jet sample (table 22): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(jet1 jet2) &lt; 1.5 and |etajet1| &lt; 2.37.

Photon+2jet sample (table 23): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(gamma jet2) &lt; 1.5, |etajet1| &lt; 2.37 and pTjet2 &lt; ETGamma.

Photon+2jet sample (table 24): ratio of cross sections in tables 22 and 23.

Photon+3jet sample (tables 25 to 29): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and pTjet3 &gt; 50 GeV.

Photon+3jet sample (tables 30, 32 and 34): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+3jet sample (tables 31, 33 and 35): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and ETGamma &gt; 300 GeV.
DOI: 10.17182/hepdata.79948.v1/t3
title: "Table 3" of "High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector"

description: Measured cross sections for isolated-photon plus 1jet production as a function of $m^{\gamma-\rm jet1}$.
description: CERN-LHC. Measurements of the cross section for prompt photon plus jet production in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.2/fb of data collected in 2012.

The photon is required to have a transverse energy above 130 GeV and absolute value of pseudorapity |etaGamma|&lt;2.37, excluding the region 1.37&lt;|etaGamma|&lt;1.56. The photon isolation is ensured by requiring the transverse energy around a cone of radius R=0.4 around the photon to be less than 10 GeV. At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons.

Jets are reconstructed using the anti-kt algorithm with radius parameter R=0.6 and required to have the jet rapidity in the range |yjet|&lt;4.4 and the distance between the jet and the photon DeltaR(gamma jet)&gt;1. The requirements on the jet transverse momenta depend on the sample and are as follows.

Photon+1jet sample (tables 1 and 2): pTjet1 &gt; 100 GeV.

Photon+1jet sample (tables 3 to 13): pTjet1 &gt; 100 GeV, |yjet1| &lt; 2.37, |costhetastar| &lt; 0.83 and |etaGamma + yjet1| &lt; 2.37 and mgammajet1 &gt; 467 GeV.

Photon+2jet sample (tables 14 to 17): pTjet1 &gt; 100 GeV and pTjet2 &gt; 65 GeV.

Photon+2jet sample (tables 18 and 20): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+2jet sample (tables 19 and 21): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and ETGamma &gt; 300 GeV.

Photon+2jet sample (table 22): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(jet1 jet2) &lt; 1.5 and |etajet1| &lt; 2.37.

Photon+2jet sample (table 23): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(gamma jet2) &lt; 1.5, |etajet1| &lt; 2.37 and pTjet2 &lt; ETGamma.

Photon+2jet sample (table 24): ratio of cross sections in tables 22 and 23.

Photon+3jet sample (tables 25 to 29): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and pTjet3 &gt; 50 GeV.

Photon+3jet sample (tables 30, 32 and 34): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+3jet sample (tables 31, 33 and 35): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and ETGamma &gt; 300 GeV.
DOI: 10.17182/hepdata.79948.v1/t4
title: "Table 4" of "High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector"

description: Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$.
description: CERN-LHC. Measurements of the cross section for prompt photon plus jet production in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.2/fb of data collected in 2012.

The photon is required to have a transverse energy above 130 GeV and absolute value of pseudorapity |etaGamma|&lt;2.37, excluding the region 1.37&lt;|etaGamma|&lt;1.56. The photon isolation is ensured by requiring the transverse energy around a cone of radius R=0.4 around the photon to be less than 10 GeV. At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons.

Jets are reconstructed using the anti-kt algorithm with radius parameter R=0.6 and required to have the jet rapidity in the range |yjet|&lt;4.4 and the distance between the jet and the photon DeltaR(gamma jet)&gt;1. The requirements on the jet transverse momenta depend on the sample and are as follows.

Photon+1jet sample (tables 1 and 2): pTjet1 &gt; 100 GeV.

Photon+1jet sample (tables 3 to 13): pTjet1 &gt; 100 GeV, |yjet1| &lt; 2.37, |costhetastar| &lt; 0.83 and |etaGamma + yjet1| &lt; 2.37 and mgammajet1 &gt; 467 GeV.

Photon+2jet sample (tables 14 to 17): pTjet1 &gt; 100 GeV and pTjet2 &gt; 65 GeV.

Photon+2jet sample (tables 18 and 20): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+2jet sample (tables 19 and 21): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and ETGamma &gt; 300 GeV.

Photon+2jet sample (table 22): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(jet1 jet2) &lt; 1.5 and |etajet1| &lt; 2.37.

Photon+2jet sample (table 23): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(gamma jet2) &lt; 1.5, |etajet1| &lt; 2.37 and pTjet2 &lt; ETGamma.

Photon+2jet sample (table 24): ratio of cross sections in tables 22 and 23.

Photon+3jet sample (tables 25 to 29): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and pTjet3 &gt; 50 GeV.

Photon+3jet sample (tables 30, 32 and 34): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+3jet sample (tables 31, 33 and 35): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and ETGamma &gt; 300 GeV.
DOI: 10.17182/hepdata.79948.v1/t5
title: "Table 5" of "High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector"

description: Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $467 &lt; m^{\gamma-\rm jet1} &lt; 510$ GeV.
description: CERN-LHC. Measurements of the cross section for prompt photon plus jet production in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.2/fb of data collected in 2012.

The photon is required to have a transverse energy above 130 GeV and absolute value of pseudorapity |etaGamma|&lt;2.37, excluding the region 1.37&lt;|etaGamma|&lt;1.56. The photon isolation is ensured by requiring the transverse energy around a cone of radius R=0.4 around the photon to be less than 10 GeV. At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons.

Jets are reconstructed using the anti-kt algorithm with radius parameter R=0.6 and required to have the jet rapidity in the range |yjet|&lt;4.4 and the distance between the jet and the photon DeltaR(gamma jet)&gt;1. The requirements on the jet transverse momenta depend on the sample and are as follows.

Photon+1jet sample (tables 1 and 2): pTjet1 &gt; 100 GeV.

Photon+1jet sample (tables 3 to 13): pTjet1 &gt; 100 GeV, |yjet1| &lt; 2.37, |costhetastar| &lt; 0.83 and |etaGamma + yjet1| &lt; 2.37 and mgammajet1 &gt; 467 GeV.

Photon+2jet sample (tables 14 to 17): pTjet1 &gt; 100 GeV and pTjet2 &gt; 65 GeV.

Photon+2jet sample (tables 18 and 20): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+2jet sample (tables 19 and 21): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and ETGamma &gt; 300 GeV.

Photon+2jet sample (table 22): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(jet1 jet2) &lt; 1.5 and |etajet1| &lt; 2.37.

Photon+2jet sample (table 23): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(gamma jet2) &lt; 1.5, |etajet1| &lt; 2.37 and pTjet2 &lt; ETGamma.

Photon+2jet sample (table 24): ratio of cross sections in tables 22 and 23.

Photon+3jet sample (tables 25 to 29): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and pTjet3 &gt; 50 GeV.

Photon+3jet sample (tables 30, 32 and 34): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+3jet sample (tables 31, 33 and 35): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and ETGamma &gt; 300 GeV.
DOI: 10.17182/hepdata.79948.v1/t6
title: "Table 6" of "High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector"

description: Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $510 &lt; m^{\gamma-\rm jet1} &lt; 590$ GeV.
description: CERN-LHC. Measurements of the cross section for prompt photon plus jet production in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.2/fb of data collected in 2012.

The photon is required to have a transverse energy above 130 GeV and absolute value of pseudorapity |etaGamma|&lt;2.37, excluding the region 1.37&lt;|etaGamma|&lt;1.56. The photon isolation is ensured by requiring the transverse energy around a cone of radius R=0.4 around the photon to be less than 10 GeV. At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons.

Jets are reconstructed using the anti-kt algorithm with radius parameter R=0.6 and required to have the jet rapidity in the range |yjet|&lt;4.4 and the distance between the jet and the photon DeltaR(gamma jet)&gt;1. The requirements on the jet transverse momenta depend on the sample and are as follows.

Photon+1jet sample (tables 1 and 2): pTjet1 &gt; 100 GeV.

Photon+1jet sample (tables 3 to 13): pTjet1 &gt; 100 GeV, |yjet1| &lt; 2.37, |costhetastar| &lt; 0.83 and |etaGamma + yjet1| &lt; 2.37 and mgammajet1 &gt; 467 GeV.

Photon+2jet sample (tables 14 to 17): pTjet1 &gt; 100 GeV and pTjet2 &gt; 65 GeV.

Photon+2jet sample (tables 18 and 20): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+2jet sample (tables 19 and 21): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and ETGamma &gt; 300 GeV.

Photon+2jet sample (table 22): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(jet1 jet2) &lt; 1.5 and |etajet1| &lt; 2.37.

Photon+2jet sample (table 23): pTjet1 &gt; 130 GeV, pTjet2 &gt; 50 GeV, Delta R(gamma jet1) &gt; 3, 1 &lt; Delta R(gamma jet2) &lt; 1.5, |etajet1| &lt; 2.37 and pTjet2 &lt; ETGamma.

Photon+2jet sample (table 24): ratio of cross sections in tables 22 and 23.

Photon+3jet sample (tables 25 to 29): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV and pTjet3 &gt; 50 GeV.

Photon+3jet sample (tables 30, 32 and 34): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and 130 &lt; ETGamma &lt; 300 GeV.

Photon+3jet sample (tables 31, 33 and 35): pTjet1 &gt; 100 GeV, pTjet2 &gt; 65 GeV, pTjet3 &gt; 50 GeV and ETGamma &gt; 300 GeV.