cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79859.v1/t15
title: "Table 15" of "Measurement of the differential cross sections for the associated production of a W boson and jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: The differential cross section measurement as a function of the azimuthal angle separation between the first leading jet and the muon.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 2.2 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, jet rapidity, the scalar sum of jet transverse momenta (HT), and angular correlations between the muon and each jet for different jet multiplicities. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.4, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.4, and only jets with pT &gt; 30 GeV, rapidity |y| &lt; 2.4, and a separation of deltaR &gt; 0.4 from the muon are considered. In addition, the differential cross section is measured as a function of the angular distance (DeltaR) between the muon and the closest jet for events with one or more jets, requiring jets with pT &gt; 100 GeV and the leading jet with pT &gt; 300 GeV.
DOI: 10.17182/hepdata.79859.v1/t16
title: "Table 16" of "Measurement of the differential cross sections for the associated production of a W boson and jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: The differential cross section measurement as a function of the azimuthal angle separation between the second leading jet and the muon.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 2.2 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, jet rapidity, the scalar sum of jet transverse momenta (HT), and angular correlations between the muon and each jet for different jet multiplicities. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.4, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.4, and only jets with pT &gt; 30 GeV, rapidity |y| &lt; 2.4, and a separation of deltaR &gt; 0.4 from the muon are considered. In addition, the differential cross section is measured as a function of the angular distance (DeltaR) between the muon and the closest jet for events with one or more jets, requiring jets with pT &gt; 100 GeV and the leading jet with pT &gt; 300 GeV.
DOI: 10.57967/hf/6877
title: OneLineCodeSnippets
DOI: 10.17182/hepdata.79859.v1/t17
title: "Table 17" of "Measurement of the differential cross sections for the associated production of a W boson and jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: The differential cross section measurement as a function of the azimuthal angle separation between the third leading jet and the muon.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 2.2 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, jet rapidity, the scalar sum of jet transverse momenta (HT), and angular correlations between the muon and each jet for different jet multiplicities. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.4, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.4, and only jets with pT &gt; 30 GeV, rapidity |y| &lt; 2.4, and a separation of deltaR &gt; 0.4 from the muon are considered. In addition, the differential cross section is measured as a function of the angular distance (DeltaR) between the muon and the closest jet for events with one or more jets, requiring jets with pT &gt; 100 GeV and the leading jet with pT &gt; 300 GeV.
DOI: 10.17182/hepdata.79859.v1/t18
title: "Table 18" of "Measurement of the differential cross sections for the associated production of a W boson and jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: The differential cross section measurement as a function of the azimuthal angle separation between the fourth leading jet and the muon.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 2.2 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, jet rapidity, the scalar sum of jet transverse momenta (HT), and angular correlations between the muon and each jet for different jet multiplicities. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.4, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.4, and only jets with pT &gt; 30 GeV, rapidity |y| &lt; 2.4, and a separation of deltaR &gt; 0.4 from the muon are considered. In addition, the differential cross section is measured as a function of the angular distance (DeltaR) between the muon and the closest jet for events with one or more jets, requiring jets with pT &gt; 100 GeV and the leading jet with pT &gt; 300 GeV.
DOI: 10.17182/hepdata.79859.v1/t19
title: "Table 19" of "Measurement of the differential cross sections for the associated production of a W boson and jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: The differential cross section measurement as a function of DeltaR separation between the muon and the closest jet for events with one or more jets.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 2.2 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, jet rapidity, the scalar sum of jet transverse momenta (HT), and angular correlations between the muon and each jet for different jet multiplicities. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.4, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.4, and only jets with pT &gt; 30 GeV, rapidity |y| &lt; 2.4, and a separation of deltaR &gt; 0.4 from the muon are considered. In addition, the differential cross section is measured as a function of the angular distance (DeltaR) between the muon and the closest jet for events with one or more jets, requiring jets with pT &gt; 100 GeV and the leading jet with pT &gt; 300 GeV.
DOI: 10.17182/hepdata.79875.v1/t1
title: "Table 1" of "Measurement of differential cross sections in the $\phi^*$ variable for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV"

description: The absolute differential cross section within the fiducial region as a function of the $\phi^*$ (phi*) variable
description: CERN-LHC. Measurements of the differential cross section for Z production as a function of $\phi^*$ (phi*) and rapidity using the 2 electron and 2 muon final states.

The fiducial region is defined as:
- 2e or 2mu
- one lepton with ptLepton &gt; 30 GeV and |etaLepton|&lt;2.1
- one lepton with ptLepton &gt; 20 GeV and |etaLepton|&lt;2.5
- mll must be between 60 and 120 GeV
DOI: 10.17182/hepdata.79875.v1/t2
title: "Table 2" of "Measurement of differential cross sections in the $\phi^*$ variable for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV"

description: The normalized differential cross section within the fiducial region as a function of the $\phi^*$ (phi*) variable
description: CERN-LHC. Measurements of the differential cross section for Z production as a function of $\phi^*$ (phi*) and rapidity using the 2 electron and 2 muon final states.

The fiducial region is defined as:
- 2e or 2mu
- one lepton with ptLepton &gt; 30 GeV and |etaLepton|&lt;2.1
- one lepton with ptLepton &gt; 20 GeV and |etaLepton|&lt;2.5
- mll must be between 60 and 120 GeV
DOI: 10.17182/hepdata.79875.v1/t3
title: "Table 3" of "Measurement of differential cross sections in the $\phi^*$ variable for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV"

description: The absolute doubly-differential cross section within the fiducial region as a function of the $\phi^*$ (phi*) variable and rapidity
description: CERN-LHC. Measurements of the differential cross section for Z production as a function of $\phi^*$ (phi*) and rapidity using the 2 electron and 2 muon final states.

The fiducial region is defined as:
- 2e or 2mu
- one lepton with ptLepton &gt; 30 GeV and |etaLepton|&lt;2.1
- one lepton with ptLepton &gt; 20 GeV and |etaLepton|&lt;2.5
- mll must be between 60 and 120 GeV
DOI: 10.17182/hepdata.79875.v1/t4
title: "Table 4" of "Measurement of differential cross sections in the $\phi^*$ variable for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV"

description: The normalized doubly-differential cross section within the fiducial region as a function of the $\phi^*$ (phi*) variable and rapidity
description: CERN-LHC. Measurements of the differential cross section for Z production as a function of $\phi^*$ (phi*) and rapidity using the 2 electron and 2 muon final states.

The fiducial region is defined as:
- 2e or 2mu
- one lepton with ptLepton &gt; 30 GeV and |etaLepton|&lt;2.1
- one lepton with ptLepton &gt; 20 GeV and |etaLepton|&lt;2.5
- mll must be between 60 and 120 GeV
DOI: 10.17182/hepdata.79875.v1/t5
title: "Additional Table 1" of "Measurement of differential cross sections in the $\phi^*$ variable for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV"

description: The covariance matrix for the absolute differential cross section within the fiducial region as a function of the $\phi^*$ (phi*) variable
description: CERN-LHC. Measurements of the differential cross section for Z production as a function of $\phi^*$ (phi*) and rapidity using the 2 electron and 2 muon final states.

The fiducial region is defined as:
- 2e or 2mu
- one lepton with ptLepton &gt; 30 GeV and |etaLepton|&lt;2.1
- one lepton with ptLepton &gt; 20 GeV and |etaLepton|&lt;2.5
- mll must be between 60 and 120 GeV
DOI: 10.17182/hepdata.79875.v1/t6
title: "Additional Table 2" of "Measurement of differential cross sections in the $\phi^*$ variable for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV"

description: The covariance matrix for the normalized differential cross section within the fiducial region as a function of the $\phi^*$ (phi*) variable
description: CERN-LHC. Measurements of the differential cross section for Z production as a function of $\phi^*$ (phi*) and rapidity using the 2 electron and 2 muon final states.

The fiducial region is defined as:
- 2e or 2mu
- one lepton with ptLepton &gt; 30 GeV and |etaLepton|&lt;2.1
- one lepton with ptLepton &gt; 20 GeV and |etaLepton|&lt;2.5
- mll must be between 60 and 120 GeV
DOI: 10.17182/hepdata.79875.v1/t7
title: "Additional Table 3" of "Measurement of differential cross sections in the $\phi^*$ variable for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV"

description: The covariance matrix for the absolute doubly-differential cross section within the fiducial region as a function of the $\phi^*$ (phi*) variable and rapidity
description: CERN-LHC. Measurements of the differential cross section for Z production as a function of $\phi^*$ (phi*) and rapidity using the 2 electron and 2 muon final states.

The fiducial region is defined as:
- 2e or 2mu
- one lepton with ptLepton &gt; 30 GeV and |etaLepton|&lt;2.1
- one lepton with ptLepton &gt; 20 GeV and |etaLepton|&lt;2.5
- mll must be between 60 and 120 GeV
DOI: 10.17182/hepdata.79875.v1/t8
title: "Additional Table 4" of "Measurement of differential cross sections in the $\phi^*$ variable for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV"

description: The covariance matrix for the normalized doubly-differential cross section within the fiducial region as a function of the $\phi^*$ (phi*) variable and rapidity
description: CERN-LHC. Measurements of the differential cross section for Z production as a function of $\phi^*$ (phi*) and rapidity using the 2 electron and 2 muon final states.

The fiducial region is defined as:
- 2e or 2mu
- one lepton with ptLepton &gt; 30 GeV and |etaLepton|&lt;2.1
- one lepton with ptLepton &gt; 20 GeV and |etaLepton|&lt;2.5
- mll must be between 60 and 120 GeV
DOI: 10.17182/hepdata.79924.v1/t1
title: "Table 1" 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 fiducial cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of a narrow-width (Γ_X = 4 MeV) spin-0 resonance as a function of its mass m_X.
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/t2
title: "Table 2" 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 fiducial cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of a spin-0 resonance as a function of its mass m_X. The decay width of the resonance equals to 2% of m_X.
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/t3
title: "Table 3" 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 fiducial cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of a spin-0 resonance as a function of its mass m_X. The decay width of the resonance equals to 6% of m_X.
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/t4
title: "Table 4" 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 fiducial cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of a narrow-width (Γ_X = 4 MeV) spin-0 resonance as a function of its mass m_X.
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/t5
title: "Table 5" 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=0.01.
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/t6
title: "Table 6" 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=0.10. Only the limits derived with the asymptotic formulae are quoted here.
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/t7
title: "Table 7" 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=0.20.
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/t10
title: "Table 10" 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-2 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.