cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.89878.v1/t43
title: "Table 43" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t44
title: "Table 44" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t45
title: "Table 45" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t46
title: "Table 46" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t47
title: "Table 47" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t48
title: "Table 48" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t49
title: "Table 49" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t50
title: "Table 50" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t51
title: "Table 51" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t52
title: "Table 52" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t53
title: "Table 53" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89878.v1/t54
title: "Table 54" of "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} =$ 13 TeV"

description: No table description available.
description: CERN-LHC. A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, $\Delta\phi_{12}$, is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 $\text{fb}^{-1}$ are used. Non-perturbative correction factors are estimated by evaluating the ratios of the predictions from PYTHIA8 tune CUETP8M1 including the simulation of multi-parton interaction and hadronization, to the predictions without considering these effects. The non-perturbative correction factors correspond to the analysis: "Azimuthal separation in nearly back-to-back jet topologies in inclusive 2- and 3-jet events in pp collisions at $\sqrt{s} = 13$ TeV".
DOI: 10.17182/hepdata.89879.v1/t1
title: "Table 1" of "Measurement of associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: The differential measurement of W + charm as a function of the absolute peudorapidity of the muon originating from the W boson.
description: CERN-LHC. Measurements are presented of associated production of a W boson and a charm quark (W + c) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 35.7 fb−1 collected by the CMS experiment at the CERN LHC. The W bosons are identified by their decay into a muon and a neutrino. The charm quarks are tagged via the full reconstruction of D∗(2010) mesons that decay via D∗(2010) --&gt; D0 + pi \to K + pi + pi. A cross section is measured in the fiducial region defined by the muon transverse momentum pT(\mu) &gt; 26 GeV, muon pseudorapidity |\eta(\mu)| &lt; 2.4, and charm quark transverse momentum pT(c) &gt; 5 GeV. The cross section is also measured differentially as a function of the pseudorapidity of the muon from the W boson decay, presented separately for W+, W- and the combination. The W + D∗(2010) cross section is determined with the additional constraint of |\eta(D*)| &lt; 2.4 and without imposing restrictions on the origin of the D∗(2010) meson.
DOI: 10.17182/hepdata.89879.v1/t2
title: "Table 2" of "Measurement of associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: The differential measurement of W+ + cbar as a function of the absolute peudorapidity of the muon originating from the W boson.
description: CERN-LHC. Measurements are presented of associated production of a W boson and a charm quark (W + c) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 35.7 fb−1 collected by the CMS experiment at the CERN LHC. The W bosons are identified by their decay into a muon and a neutrino. The charm quarks are tagged via the full reconstruction of D∗(2010) mesons that decay via D∗(2010) --&gt; D0 + pi \to K + pi + pi. A cross section is measured in the fiducial region defined by the muon transverse momentum pT(\mu) &gt; 26 GeV, muon pseudorapidity |\eta(\mu)| &lt; 2.4, and charm quark transverse momentum pT(c) &gt; 5 GeV. The cross section is also measured differentially as a function of the pseudorapidity of the muon from the W boson decay, presented separately for W+, W- and the combination. The W + D∗(2010) cross section is determined with the additional constraint of |\eta(D*)| &lt; 2.4 and without imposing restrictions on the origin of the D∗(2010) meson.
DOI: 10.17182/hepdata.89879.v1/t3
title: "Table 3" of "Measurement of associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: The differential measurement of W- + c as a function of the absolute peudorapidity of the muon originating from the W boson.
description: CERN-LHC. Measurements are presented of associated production of a W boson and a charm quark (W + c) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 35.7 fb−1 collected by the CMS experiment at the CERN LHC. The W bosons are identified by their decay into a muon and a neutrino. The charm quarks are tagged via the full reconstruction of D∗(2010) mesons that decay via D∗(2010) --&gt; D0 + pi \to K + pi + pi. A cross section is measured in the fiducial region defined by the muon transverse momentum pT(\mu) &gt; 26 GeV, muon pseudorapidity |\eta(\mu)| &lt; 2.4, and charm quark transverse momentum pT(c) &gt; 5 GeV. The cross section is also measured differentially as a function of the pseudorapidity of the muon from the W boson decay, presented separately for W+, W- and the combination. The W + D∗(2010) cross section is determined with the additional constraint of |\eta(D*)| &lt; 2.4 and without imposing restrictions on the origin of the D∗(2010) meson.
DOI: 10.17182/hepdata.89879.v1/t4
title: "Table 4" of "Measurement of associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: The differential measurement of W + D*(2010) as a function of the absolute peudorapidity of the muon originating from the W boson.
description: CERN-LHC. Measurements are presented of associated production of a W boson and a charm quark (W + c) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 35.7 fb−1 collected by the CMS experiment at the CERN LHC. The W bosons are identified by their decay into a muon and a neutrino. The charm quarks are tagged via the full reconstruction of D∗(2010) mesons that decay via D∗(2010) --&gt; D0 + pi \to K + pi + pi. A cross section is measured in the fiducial region defined by the muon transverse momentum pT(\mu) &gt; 26 GeV, muon pseudorapidity |\eta(\mu)| &lt; 2.4, and charm quark transverse momentum pT(c) &gt; 5 GeV. The cross section is also measured differentially as a function of the pseudorapidity of the muon from the W boson decay, presented separately for W+, W- and the combination. The W + D∗(2010) cross section is determined with the additional constraint of |\eta(D*)| &lt; 2.4 and without imposing restrictions on the origin of the D∗(2010) meson.
DOI: 10.17182/hepdata.89879.v1/t5
title: "Table 5" of "Measurement of associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: The differential measurement of W+ + D*(2010)- as a function of the absolute peudorapidity of the muon originating from the W boson.
description: CERN-LHC. Measurements are presented of associated production of a W boson and a charm quark (W + c) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 35.7 fb−1 collected by the CMS experiment at the CERN LHC. The W bosons are identified by their decay into a muon and a neutrino. The charm quarks are tagged via the full reconstruction of D∗(2010) mesons that decay via D∗(2010) --&gt; D0 + pi \to K + pi + pi. A cross section is measured in the fiducial region defined by the muon transverse momentum pT(\mu) &gt; 26 GeV, muon pseudorapidity |\eta(\mu)| &lt; 2.4, and charm quark transverse momentum pT(c) &gt; 5 GeV. The cross section is also measured differentially as a function of the pseudorapidity of the muon from the W boson decay, presented separately for W+, W- and the combination. The W + D∗(2010) cross section is determined with the additional constraint of |\eta(D*)| &lt; 2.4 and without imposing restrictions on the origin of the D∗(2010) meson.
DOI: 10.17182/hepdata.89879.v1/t6
title: "Table 6" of "Measurement of associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: The differential measurement of W- + D*(2010)+ as a function of the absolute peudorapidity of the muon originating from the W boson.
description: CERN-LHC. Measurements are presented of associated production of a W boson and a charm quark (W + c) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 35.7 fb−1 collected by the CMS experiment at the CERN LHC. The W bosons are identified by their decay into a muon and a neutrino. The charm quarks are tagged via the full reconstruction of D∗(2010) mesons that decay via D∗(2010) --&gt; D0 + pi \to K + pi + pi. A cross section is measured in the fiducial region defined by the muon transverse momentum pT(\mu) &gt; 26 GeV, muon pseudorapidity |\eta(\mu)| &lt; 2.4, and charm quark transverse momentum pT(c) &gt; 5 GeV. The cross section is also measured differentially as a function of the pseudorapidity of the muon from the W boson decay, presented separately for W+, W- and the combination. The W + D∗(2010) cross section is determined with the additional constraint of |\eta(D*)| &lt; 2.4 and without imposing restrictions on the origin of the D∗(2010) meson.
DOI: 10.17182/hepdata.89880.v1/t1
title: "Figure 2a(AuAu)" of "Jet-Hadron Correlations in sqrt{s_{NN}} = 200 GeV Au+Au and p+p Collisions"

description: Jet-hadron correlations after background subtraction. Shown with Gaussian fits to jet peaks and systematic uncertanty bands Au+Au(0.5-1 GeV).
description: BNL-RHIC. Azimuthal angular correlations of charged hadrons with respect to the axis of a reconstructed (trigger) jet in Au+Au and p+p collisions at sNN−−−sqrt=200GeV in STAR are presented. The trigger jet population in Au+Au collisions is biased towards jets that have not interacted with the medium, allowing easier matching of jet energies between Au+Au and p+p collisions while enhancing medium effects on the recoil jet. The associated hadron yield of the recoil jet is significantly suppressed at high transverse momentum (passocT) and enhanced at low passocT in 0-20% central Au+Au collisions compared to p+p collisions, which is indicative of medium-induced parton energy loss in ultrarelativistic heavy-ion collisions.