cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.146028.v1/t21
title: "Figure11a" 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 NNPDF31NNLO 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/t22
title: "Figure11b" 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 NNPDF31NNLO 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/t23
title: "Figure11c" 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 NNPDF31NNLO 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/t24
title: "Figure11d" 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 NNPDF31NNLO 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/t25
title: "Figure12a" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: The effect of aS(MZ) variation, for |y|&lt;0.5. The NNLO theoretical cross section predictions using the NNPDF31NNLO PDF with m = HT, calculated for different choices of aS (0.108, 0.110, 0.112, 0.114, 0.116, 0.117, 0.118, 0.119, 0.120, 0.122, and 0.124), are divided by the benchmark NNLO prediction for aS = 0.118 and the same choice of PDF set, muR, and muF. Also shown is the experimental unfolded measurement divided by the same benchmark prediction. The width of the unity line corresponds to the statistical uncertainty from the MC integration for the determination of the NNLO prediction. The error bars on the unfolded data correspond to the total experimental statistical and systematic uncertainty added in quadrature.
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/t26
title: "Figure12b" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: The effect of aS(MZ) variation, for 0.5&lt;|y|&lt;1. The NNLO theoretical cross section predictions using the NNPDF31NNLO PDF with m = HT, calculated for different choices of aS (0.108, 0.110, 0.112, 0.114, 0.116, 0.117, 0.118, 0.119, 0.120, 0.122, and 0.124), are divided by the benchmark NNLO prediction for aS = 0.118 and the same choice of PDF set, muR, and muF. Also shown is the experimental unfolded measurement divided by the same benchmark prediction. The width of the unity line corresponds to the statistical uncertainty from the MC integration for the determination of the NNLO prediction. The error bars on the unfolded data correspond to the total experimental statistical and systematic uncertainty added in quadrature.
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/t27
title: "Figure12c" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: The effect of aS(MZ) variation, for 1&lt;|y|&lt;1.5. The NNLO theoretical cross section predictions using the NNPDF31NNLO PDF with m = HT, calculated for different choices of aS (0.108, 0.110, 0.112, 0.114, 0.116, 0.117, 0.118, 0.119, 0.120, 0.122, and 0.124), are divided by the benchmark NNLO prediction for aS = 0.118 and the same choice of PDF set, muR, and muF. Also shown is the experimental unfolded measurement divided by the same benchmark prediction. The width of the unity line corresponds to the statistical uncertainty from the MC integration for the determination of the NNLO prediction. The error bars on the unfolded data correspond to the total experimental statistical and systematic uncertainty added in quadrature.
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/t28
title: "Figure12d" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: The effect of aS(MZ) variation, for 1.5&lt;|y|&lt;2. The NNLO theoretical cross section predictions using the NNPDF31NNLO PDF with m = HT, calculated for different choices of aS (0.108, 0.110, 0.112, 0.114, 0.116, 0.117, 0.118, 0.119, 0.120, 0.122, and 0.124), are divided by the benchmark NNLO prediction for aS = 0.118 and the same choice of PDF set, muR, and muF. Also shown is the experimental unfolded measurement divided by the same benchmark prediction. The width of the unity line corresponds to the statistical uncertainty from the MC integration for the determination of the NNLO prediction. The error bars on the unfolded data correspond to the total experimental statistical and systematic uncertainty added in quadrature.
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/t29
title: "unfoldcorrmat_1" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Unfolded correlation matrix for |y|&lt;0.5.
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/t30
title: "unfoldcorrmat_2" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Unfolded correlation matrix for 0.5&lt;|y|&lt;1.
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/t31
title: "unfoldcorrmat_3" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Unfolded correlation matrix for 1&lt;|y|&lt;1.5.
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/t32
title: "unfoldcorrmat_4" of "Measurement of the double-differential inclusive jet cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV"

description: Unfolded correlation matrix for 1.5&lt;|y|&lt;2.
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.146074.v1/t1
title: "Figure 3-a" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison of data and background pT distribution at the preselection level for the first leading muon.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t2
title: "Figure 3-b" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison of data and background pT distribution at the preselection level for the second leading muon.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t3
title: "Figure 3-c" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison of data and background pT distribution at the preselection level for the first leading jet.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t4
title: "Figure 3-d" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison of data and background pT distribution at the preselection level for the second leading jet.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t5
title: "Figure 4-a" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison of data and background BDT discriminant distributions at the preselection level for LQ mass hypotheses of 1500 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t6
title: "Figure 4-b" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison of data and background BDT discriminant distributions at the preselection level for LQ mass hypotheses of 1800 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t7
title: "Figure 4-c" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison of data and background BDT discriminant distributions at the preselection level for LQ mass hypotheses of 2000 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t8
title: "Figure 5" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Total signal selection efficiency, defined as the number of events passing the selection divided by the number of generated events. Enhanced preselection is defined as preselection with the additional requirements m_uu&gt;250 and m_uujj&gt;m_lq. The discrete nature of the final selection for each LQ candidate mass produces the observed variation in the efficiency. Relative uncertainties are less than one percent in all cases.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t10
title: "Figure 7" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The expected and observed upper limits at 95% CL on the product of the scalar LQ pair production cross section and the branching fractions β^2 as a function of mLQ. The solid lines represent the observed limits, the dashed lines represent the median expected limits, and the inner dark-green and outer light-yellow bands represent the 68% and 95% CL intervals. The σtheory curves and their blue bands represent the theoretical scalar LQ pair production cross sections and the uncertainties on the cross sections due to the PDF prediction and renormalization and factorization scales, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t11
title: "Figure 8" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The expected and observed exclusion limits at 95% CL as a function of the leptoquark mass and the branching fraction β. The solid line represents the observed limits, the dashed line represents the median expected limits, and the inner dark-green and outer light-yellow bands represent the 68% and 95% CL intervals. The area below the observed limit is excluded.
description: No data abstract available.
DOI: 10.17182/hepdata.146074.v1/t9
title: "Event Count Table" of "Search for pair production of scalar and vector leptoquarks decaying to muons and bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Event yields in the combined 2016--2018 data at the final selection level.
description: No data abstract available.