cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.167810.v1/t1
title: "Figure 1a" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Complement of transverse thrust($\tau_{\perp}$) for $83
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t10
title: "Figure 2b" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Three-jet resolution parameter($Y_{23}$) for $109
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t11
title: "Figure 2c" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Three-jet resolution parameter($Y_{23}$) for $176
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t13
title: "Figure 2e" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Three-jet resolution parameter($Y_{23}$) for $318
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t2
title: "Figure 1b" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Complement of transverse thrust($\tau_{\perp}$) for $109
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t3
title: "Figure 1c" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Complement of transverse thrust($\tau_{\perp}$) for $176
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t4
title: "Figure 1d" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Complement of transverse thrust($\tau_{\perp}$) for $247
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t5
title: "Figure 1e" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Complement of transverse thrust($\tau_{\perp}$) for $318
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t12
title: "Figure 2d" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Three-jet resolution parameter($Y_{23}$) for $247
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t14
title: "Figure 2f" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Three-jet resolution parameter($Y_{23}$) for $387
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t15
title: "Figure 2g" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Three-jet resolution parameter($Y_{23}$) for $477
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t16
title: "Figure 2h" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Three-jet resolution parameter($Y_{23}$) for $H_{T,2}&gt;573$ GeV
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t17
title: "Figure 3a" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet broadening($B_{tot}$) for $83
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t18
title: "Figure 3b" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet broadening($B_{tot}$) for $109
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t19
title: "Figure 3c" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet broadening($B_{tot}$) for $176
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t20
title: "Figure 3d" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet broadening($B_{tot}$) for $247
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t21
title: "Figure 3e" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet broadening($B_{tot}$) for $318
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t22
title: "Figure 3f" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet broadening($B_{tot}$) for $387
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t23
title: "Figure 3g" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet broadening($B_{tot}$) for $477
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t24
title: "Figure 3h" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet broadening($B_{tot}$) for $H_{T,2}&gt;573$ GeV
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t25
title: "Figure 4a" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet mass($\rho_{tot}$) for $83
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t26
title: "Figure 4b" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet mass($\rho_{tot}$) for $109
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.
DOI: 10.17182/hepdata.167810.v1/t28
title: "Figure 4d" of "Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized unfolded distributions of Total jet mass($\rho_{tot}$) for $247
description: CERN-LHC. Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016--2018, corresponding to an integrated luminosity of 138 $fb^{-1}$. The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the results from the predictions from a number of models for multijet production. Overall, there is general agreement between several theoretical predictions and the data.