cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.146028.v1/t6
title: "Figure7b" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: The unfolded measured particle-level inclusive jet cross section as functions of jet pT (markers), for 0.5&lt;|y|&lt;1, compared to the NLO perturbative QCD prediction (histogram), using the CT14NLO PDF set, with muR = muF = HT, and corrected for the NP effects. The experimental and theoretical systematic uncertainties are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t10
title: "Figure8b" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NLO theoretical predictions, using the CT14NLO PDF set, with mu = pT, for 0.5&lt;|y|&lt;1. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t11
title: "Figure8c" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NLO theoretical predictions, using the CT14NLO PDF set, with mu = pT, for 1&lt;|y|&lt;1.5. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t7
title: "Figure7c" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: The unfolded measured particle-level inclusive jet cross section as functions of jet pT (markers), for 1&lt;|y|&lt;1.5, compared to the NLO perturbative QCD prediction (histogram), using the CT14NLO PDF set, with muR = muF = HT, and corrected for the NP effects. The experimental and theoretical systematic uncertainties are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t8
title: "Figure7d" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: The unfolded measured particle-level inclusive jet cross section as functions of jet pT (markers), for 1.5&lt;|y|&lt;2, compared to the NLO perturbative QCD prediction (histogram), using the CT14NLO PDF set, with muR = muF = HT, and corrected for the NP effects. The experimental and theoretical systematic uncertainties are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t9
title: "Figure8a" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NLO theoretical predictions, using the CT14NLO PDF set, with mu = pT, for |y|&lt;0.5. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t12
title: "Figure8d" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NLO theoretical predictions, using the CT14NLO PDF set, with mu = pT, for 1.5&lt;|y|&lt;2. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t13
title: "Figure9a" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NLO theoretical predictions, using the CT14NLO PDF set, with mu = HT, for |y|&lt;0.5. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t14
title: "Figure9b" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NLO theoretical predictions, using the CT14NLO PDF set, with mu = HT, for 0.5&lt;|y|&lt;1. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t15
title: "Figure9c" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NLO theoretical predictions, using the CT14NLO PDF set, with mu = HT, for 1&lt;|y|&lt;1.5. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t16
title: "Figure9d" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NLO theoretical predictions, using the CT14NLO PDF set, with mu = HT, for 1.5&lt;|y|&lt;2. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t17
title: "Figure10a" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NNLO theoretical predictions, using the CT14NNLO PDF set, with mu = HT, for |y|&lt;0.5. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t18
title: "Figure10b" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NNLO theoretical predictions, using the CT14NNLO PDF set, with mu = HT, for 0.5&lt;|y|&lt;1. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t19
title: "Figure10c" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NNLO theoretical predictions, using the CT14NNLO PDF set, with mu = HT, for 1&lt;|y|&lt;1.5. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.
DOI: 10.17182/hepdata.146028.v1/t20
title: "Figure10d" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Ratios (points) of the unfolded measured cross sections to the NNLO theoretical predictions, using the CT14NNLO PDF set, with mu = HT, for 1.5&lt;|y|&lt;2. The vertical error bars show the statistical experimental uncertainty. The systematic experimental uncertainty, the total theoretical uncertainty, and the individual sources of theoretical uncertainty are shown.
description: The inclusive jet cross section is measured as a function of jet transverse momentum $p_T$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} = 5.02$ TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_{\rm T}$ algorithm using a distance parameter of $R=0.4$, within the rapidity interval $|y| &lt; 2$, and across the kinematic range $0.06 &lt; $p_T$ &lt; 1$ TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_{\rm S}$.