cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.146075.v1/t15
title: "NP_3D_Mass_AK8" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Nonperturbative corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t16
title: "StatCorr_3D_Mass_AK8" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Statistical correlation coefficients for triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t17
title: "CrossSection_3D_PtAve_AK4" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t18
title: "EW_3D_PtAve_AK4" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Electroweak corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t19
title: "NP_3D_PtAve_AK4" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Nonperturbative corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t20
title: "StatCorr_3D_PtAve_AK4" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Statistical correlation coefficients for triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t21
title: "CrossSection_3D_PtAve_AK8" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t22
title: "EW_3D_PtAve_AK8" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Electroweak corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t23
title: "NP_3D_PtAve_AK8" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Nonperturbative corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146075.v1/t24
title: "StatCorr_3D_PtAve_AK8" of "Measurement of multidifferential cross sections for dijet production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Statistical correlation coefficients for triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)
description: A measurement of the dijet production cross section is reported based on proton-proton collision data collected in 2016 at $\sqrt{s}$ = 13 TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3 fb$^{-1}$. Jets are reconstructed with the anti-$k_\text{T}$ algorithm for distance parameters of $R$ = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity $\left| y \right|_\text{max}$ of the two jets with the highest transverse momenta $p_\text{T}$ and their invariant mass $m_{1,2}$, and triple-differentially (3D) as a function of the rapidity separation $y^{*}$, the total boost $y_\text{b}$, and either $m_{1,2}$ or the average $p_\text{T}$ of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of $\alpha_\text{s}(m_\text{Z})=0.1179\pm0.0019$.
DOI: 10.17182/hepdata.146076.v1/t1
title: "Table 1a" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 0-1\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t2
title: "Table 1b" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 1-5\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t3
title: "Table 1c" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 5-10\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t4
title: "Table 1d" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 10-20\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t5
title: "Table 1e" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 20-30\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t6
title: "Table 1f" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 30-40\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t7
title: "Table 1g" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 40-50\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t8
title: "Table 1h" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 50-70\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t9
title: "Table 1i" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 70-100\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t10
title: "Table 1j" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 0-100\% multiplicity class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t11
title: "Table 2a" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe Xe collisions at \sqrt{s_{NN}}$ = 5.44 TeV for 0-30\% centrality class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t12
title: "Table 2b" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe Xe collisions at \sqrt{s_{NN}}$ = 5.44 TeV for 30-50\% centrality class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t13
title: "Table 2c" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe Xe collisions at \sqrt{s_{NN}}$ = 5.44 TeV for 50-70\% centrality class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t14
title: "Table 2d" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe Xe collisions at \sqrt{s_{NN}}$ = 5.44 TeV for 70-90\% centrality class.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t15
title: "Table 3" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-integrated yield d$N$/d$y$ of K$^{*}$ (average of particle and anti-particle) meson measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t16
title: "Table 4" of "System size dependence of hadronic rescattering effect at LHC energies"

description: Mean $p_{\rm T}$ of K$^{*}$ (average of particle and anti-particle) meson measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t17
title: "Table 5" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-integrated yield d$N$/d$y$ of K$^{*}$ (average of particle and anti-particle) meson measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t18
title: "Table 6" of "System size dependence of hadronic rescattering effect at LHC energies"

description: Mean $p_{\rm T}$ of K$^{*}$ (average of particle and anti-particle) meson measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t19
title: "Table 7" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-integrated yield ratio of $\rm{K}^{*}$ (average of particleand anti-particle) to K (average of particle and anti-particle) measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t20
title: "Table 8" of "System size dependence of hadronic rescattering effect at LHC energies"

description: $p_{\rm T}$-integrated yield ratio of $\rm{K}^{*}$ (average of particleand anti-particle) to K (average of particle and anti-particle) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146076.v1/t21
title: "Table 9" of "System size dependence of hadronic rescattering effect at LHC energies"

description: Lower limit of the hadronic phase lifetime measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.
description: No data abstract available.