cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79948.v1/t34
title: "Table 34" 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 3jet production as a function of $\Delta\phi^{\rm jet2-jet3}$ for the range $130&lt; E_{\rm T}^{\gamma} &lt;300$ 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/t35
title: "Table 35" 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 3jet production as a function of $\Delta\phi^{\rm jet2-jet3}$ for the range $E_{\rm T}^{\gamma} &gt;300$ 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.79950.v1/t1
title: "Table 1" of "Measurement of $W^+W^-$ production in association with one jet in proton--proton collisions at $\sqrt{s} =8$ TeV with the ATLAS detector"

description: Measured production cross section of WW production in the fiducial region in case one W boson decays into a prompt electron and the other one into a prompt muon. The cross section is defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)&lt;2.47 and to lie outside of 1.37 &lt; abs(eta) &lt; 1.53, muons are required to lie within abs(eta)&lt;2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. 
The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 20 GeV (PT(C=SUM(NU))). The transverse momentum of the vectorial sum of the neutrinos is multiplied by the sine of the azimuthal difference between lepton and the vectorial sum of the neutrinos if their azimuthal difference is smaller than PI/2. It is required to be larger than 15 GeV. 
The invariant mass of the leptons should exceed 10 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. Only events with exactly one jet above 25 GeV and within abs(eta)&lt;4.5 are selected. Events containing b-jets with p T &gt; 20 GeV and within |η| &lt; 2.5 are rejected. Both, resonant and non-resonant WW production processes, are included in the cross sections.
description: No data abstract available.
DOI: 10.17182/hepdata.79950.v1/t2
title: "Table 2" of "Measurement of $W^+W^-$ production in association with one jet in proton--proton collisions at $\sqrt{s} =8$ TeV with the ATLAS detector"

description: Measured production cross section of WW production in the fiducial region in case one W boson decays into a prompt electron and the other one into a prompt muon. The cross section is defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)&lt;2.47 and to lie outside of 1.37 &lt; abs(eta) &lt; 1.53, muons are required to lie within abs(eta)&lt;2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. 
The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 20 GeV (PT(C=SUM(NU))). The transverse momentum of the vectorial sum of the neutrinos is multiplied by the sine of the azimuthal difference between lepton and the vectorial sum of the neutrinos if their azimuthal difference is smaller than PI/2. It is required to be larger than 15 GeV. 
The invariant mass of the leptons should exceed 10 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. Only events with zero or exactly one jet above 25 GeV and within abs(eta)&lt;4.5 are selected. Events containing b-jets with p T &gt; 20 GeV and within |η| &lt; 2.5 are rejected. Both, resonant and non-resonant WW production processes, are included in the cross sections.
description: No data abstract available.
DOI: 10.17182/hepdata.79950.v1/t3
title: "Table 3" of "Measurement of $W^+W^-$ production in association with one jet in proton--proton collisions at $\sqrt{s} =8$ TeV with the ATLAS detector"

description: Measured ratio of the production cross section of WW production with
one associated jet to the production cross section of WW production with
zero associated jets. The ratio is determined in the in the fiducial region which is defined in case one W boson decays into a prompt electron and the other one into a prompt muon. The cross section is defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)&lt;2.47 and to lie outside of 1.37 &lt; abs(eta) &lt; 1.53, muons are required to lie within abs(eta)&lt;2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. 
The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 20 GeV (PT(C=SUM(NU))). The transverse momentum of the vectorial sum of the neutrinos is multiplied by the sine of the azimuthal difference between lepton and the vectorial sum of the neutrinos if their azimuthal difference is smaller than PI/2. It is required to be larger than 15 GeV. 
The invariant mass of the leptons should exceed 10 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. Only events with zero or exactly one jet above 25 GeV and within abs(eta)&lt;4.5 are selected. Events containing b-jets with p T &gt; 20 GeV and within |η| &lt; 2.5 are rejected. Both, resonant and non-resonant WW production processes, are included in the cross sections.
description: No data abstract available.
DOI: 10.17182/hepdata.79950.v1/t4
title: "Table 4" of "Measurement of $W^+W^-$ production in association with one jet in proton--proton collisions at $\sqrt{s} =8$ TeV with the ATLAS detector"

description: Measured total production cross sections of WW production in the total phase space. Both, resonant and non-resonant WW, production are considered as signal.
description: No data abstract available.
DOI: 10.17182/hepdata.79951.v1/t1
title: "Table 1" of "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector"

description: Observed allowed ranges for 6 dimensional aQGCs, cutoff 500 GeV.
description: ATLAS CERN-LHC. Measurements of exclusive electron muon events in ATLAS at 8

TeV are used to estimate the exclusive cross section for W+W-, put limits on 

anomolous quartic couplings (aQGCs), and limit the cross section for 

diffractive Higgs production. The fiducial region is defined as 

- |etaLepton| &lt;2.5
- ptLepton &gt;25 (second lepton &gt;20 or &gt;15 for Higgs study)
- exclusivity no other track associated with the electron/muon intersection with pt &gt;0.5

The luminosity is 20.2 (0.4) 1/fb at 8 TeV. Calibration of exclusivity is

data based and e e and mu mu results agree with previous measurements.

The results are

- dimuons &gt; 160 GeV/c2 ratio observed/elastic predicted 3.30 (0.22) (0.06)
- WW sigmaB emuX (gamma gamma) 6.9 (2.2) (1.4) pb consistent with expectation 
- anomolous expect pt(emu) &gt;120 expect 0.4 see 1, limits on dim 6 and 8
- Higgs selection expect 3 see 6, UL 95% 1.2 pb
DOI: 10.17182/hepdata.79951.v1/t2
title: "Table 2" of "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector"

description: Expected allowed ranges for 6 dimensional aQGCs, no cutoff).
description: ATLAS CERN-LHC. Measurements of exclusive electron muon events in ATLAS at 8

TeV are used to estimate the exclusive cross section for W+W-, put limits on 

anomolous quartic couplings (aQGCs), and limit the cross section for 

diffractive Higgs production. The fiducial region is defined as 

- |etaLepton| &lt;2.5
- ptLepton &gt;25 (second lepton &gt;20 or &gt;15 for Higgs study)
- exclusivity no other track associated with the electron/muon intersection with pt &gt;0.5

The luminosity is 20.2 (0.4) 1/fb at 8 TeV. Calibration of exclusivity is

data based and e e and mu mu results agree with previous measurements.

The results are

- dimuons &gt; 160 GeV/c2 ratio observed/elastic predicted 3.30 (0.22) (0.06)
- WW sigmaB emuX (gamma gamma) 6.9 (2.2) (1.4) pb consistent with expectation 
- anomolous expect pt(emu) &gt;120 expect 0.4 see 1, limits on dim 6 and 8
- Higgs selection expect 3 see 6, UL 95% 1.2 pb
DOI: 10.17182/hepdata.79951.v1/t3
title: "Table 3" of "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector"

description: Observed allowed ranges for 8 dimensional aQGCs, cutoff 500).
description: ATLAS CERN-LHC. Measurements of exclusive electron muon events in ATLAS at 8

TeV are used to estimate the exclusive cross section for W+W-, put limits on 

anomolous quartic couplings (aQGCs), and limit the cross section for 

diffractive Higgs production. The fiducial region is defined as 

- |etaLepton| &lt;2.5
- ptLepton &gt;25 (second lepton &gt;20 or &gt;15 for Higgs study)
- exclusivity no other track associated with the electron/muon intersection with pt &gt;0.5

The luminosity is 20.2 (0.4) 1/fb at 8 TeV. Calibration of exclusivity is

data based and e e and mu mu results agree with previous measurements.

The results are

- dimuons &gt; 160 GeV/c2 ratio observed/elastic predicted 3.30 (0.22) (0.06)
- WW sigmaB emuX (gamma gamma) 6.9 (2.2) (1.4) pb consistent with expectation 
- anomolous expect pt(emu) &gt;120 expect 0.4 see 1, limits on dim 6 and 8
- Higgs selection expect 3 see 6, UL 95% 1.2 pb
DOI: 10.17182/hepdata.79951.v1/t4
title: "Table 4" of "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector"

description: Expected allowed ranges for 8 dimensional aQGC, no cutoff).
description: ATLAS CERN-LHC. Measurements of exclusive electron muon events in ATLAS at 8

TeV are used to estimate the exclusive cross section for W+W-, put limits on 

anomolous quartic couplings (aQGCs), and limit the cross section for 

diffractive Higgs production. The fiducial region is defined as 

- |etaLepton| &lt;2.5
- ptLepton &gt;25 (second lepton &gt;20 or &gt;15 for Higgs study)
- exclusivity no other track associated with the electron/muon intersection with pt &gt;0.5

The luminosity is 20.2 (0.4) 1/fb at 8 TeV. Calibration of exclusivity is

data based and e e and mu mu results agree with previous measurements.

The results are

- dimuons &gt; 160 GeV/c2 ratio observed/elastic predicted 3.30 (0.22) (0.06)
- WW sigmaB emuX (gamma gamma) 6.9 (2.2) (1.4) pb consistent with expectation 
- anomolous expect pt(emu) &gt;120 expect 0.4 see 1, limits on dim 6 and 8
- Higgs selection expect 3 see 6, UL 95% 1.2 pb
DOI: 10.17182/hepdata.79951.v1/t5
title: "Table 5" of "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector"

description: Inclusive Cross Section.
description: ATLAS CERN-LHC. Measurements of exclusive electron muon events in ATLAS at 8

TeV are used to estimate the exclusive cross section for W+W-, put limits on 

anomolous quartic couplings (aQGCs), and limit the cross section for 

diffractive Higgs production. The fiducial region is defined as 

- |etaLepton| &lt;2.5
- ptLepton &gt;25 (second lepton &gt;20 or &gt;15 for Higgs study)
- exclusivity no other track associated with the electron/muon intersection with pt &gt;0.5

The luminosity is 20.2 (0.4) 1/fb at 8 TeV. Calibration of exclusivity is

data based and e e and mu mu results agree with previous measurements.

The results are

- dimuons &gt; 160 GeV/c2 ratio observed/elastic predicted 3.30 (0.22) (0.06)
- WW sigmaB emuX (gamma gamma) 6.9 (2.2) (1.4) pb consistent with expectation 
- anomolous expect pt(emu) &gt;120 expect 0.4 see 1, limits on dim 6 and 8
- Higgs selection expect 3 see 6, UL 95% 1.2 pb
DOI: 10.17182/hepdata.79953.v2/t1
title: "Table 1" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from Fig 3a. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) &gt; 600 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 &lt; log_{10}(\rho^2) &lt; -1.7$.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t2
title: "Table 2" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from Fig 3b. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) &gt; 600 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 &lt; log_{10}(\rho^2) &lt; -1.7$.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t3
title: "Table 3" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from Fig 3c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) &gt; 600 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 &lt; log_{10}(\rho^2) &lt; -1.7$. The uncertainties are applied symmetrically, though the cross section cannot go below zero in the first bin.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t10
title: "Table 10" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from FigAux 7a. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 0, inclusive in $p_T$.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t11
title: "Table 11" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from FigAux 7b. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 1, inclusive in $p_T$.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t4
title: "Table 4" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from FigAux 4 and FigAux 8a-16a. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) &gt; 600 GeV, after the soft drop algorithm is applied for beta = 0, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 &lt; log_{10}(\rho^2) &lt; -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t5
title: "Table 5" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from FigAux 4 and FigAux 8b-16b. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) &gt; 600 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 &lt; log_{10}(\rho^2) &lt; -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t6
title: "Table 6" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from FigAux 8c-16c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) &gt; 600 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 &lt; log_{10}(\rho^2) &lt; -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t7
title: "Table 7" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from FigAux 6a. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 0. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.79953.v2/t8
title: "Table 8" of "A measurement of the soft-drop jet mass in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Data from FigAux 6b. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 1. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
description: Unfolded soft drop jet mass distributions for dijet events.