cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79410.v1/t9
title: "Table 5" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t11
title: "Table 6" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t13
title: "Table 13" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Electroweak correction factor to triple-differential dijet cross section
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t15
title: "Table 15" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Electroweak correction factor to triple-differential dijet cross section
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t16
title: "Table 16" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Electroweak correction factor to triple-differential dijet cross section
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t17
title: "Table 17" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Electroweak correction factor to triple-differential dijet cross section
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t18
title: "Table 18" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Electroweak correction factor to triple-differential dijet cross section
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t19
title: "Table 19" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Nonperturbative correction factor to triple-differential dijet cross section with uncertainty
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t20
title: "Table 20" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Nonperturbative correction factor to triple-differential dijet cross section with uncertainty
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t21
title: "Table 21" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Nonperturbative correction factor to triple-differential dijet cross section with uncertainty
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t22
title: "Table 22" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Nonperturbative correction factor to triple-differential dijet cross section with uncertainty
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t23
title: "Table 23" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Nonperturbative correction factor to triple-differential dijet cross section with uncertainty
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t24
title: "Table 24" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Nonperturbative correction factor to triple-differential dijet cross section with uncertainty
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79411.v1/t1
title: "Table 1" of "Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings"

description: The W+W- production cross section combining the four event categories (different-flavor and same-flavor in the 0-jet and 1-jet bin separately) by performing a profile likelihood fit to the data.
description: CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data 
collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are
selected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the 
normalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. 
Limits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective 
field theory.
DOI: 10.17182/hepdata.79411.v1/t2
title: "Table 2" of "Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings"

description: The W+W- production cross section in fiducial regions defined by requiring no jets at particle level with jet pT thresholds as listed.
description: CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data 
collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are
selected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the 
normalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. 
Limits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective 
field theory.
DOI: 10.17182/hepdata.79411.v1/t3
title: "Table 3" of "Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings"

description: The W+W- production cross section in fiducial regions defined by requiring zero jets at particle level with varying jet pT thresholds and requiring prompt leptons with pT &gt; 20 GeV and abs(eta) &lt; 2.5, before final-state radiation.
description: CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data 
collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are
selected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the 
normalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. 
Limits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective 
field theory.
DOI: 10.17182/hepdata.79411.v1/t4
title: "Table 4" of "Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings"

description: Normalized differential W+W- cross section as a function of the leading lepton pT. Both statistical and systematic uncertainties are included. Results are computed in a fiducial region defined by requiring zero jets at particle level with varying jet pT thresholds and requiring prompt leptons with pT &gt; 20 GeV and abs(eta) &lt; 2.5, before final-state radiation.
description: CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data 
collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are
selected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the 
normalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. 
Limits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective 
field theory.
DOI: 10.17182/hepdata.79411.v1/t5
title: "Table 5" of "Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings"

description: Normalized differential W+W- cross section as a function of the dilepton system. Both statistical and systematic uncertainties are included. Results are computed in a fiducial region defined by requiring zero jets at particle level with varying jet pT thresholds and requiring prompt leptons with pT &gt; 20 GeV and abs(eta) &lt; 2.5, before final-state radiation.
description: CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data 
collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are
selected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the 
normalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. 
Limits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective 
field theory.
DOI: 10.17182/hepdata.79411.v1/t6
title: "Table 6" of "Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings"

description: Normalized differential W+W- cross section as a function of the invariant mass. Both statistical and systematic uncertainties are included. Results are computed in a fiducial region defined by requiring zero jets at particle level with varying jet pT thresholds and requiring prompt leptons with pT &gt; 20 GeV and abs(eta) &lt; 2.5, before final-state radiation.
description: CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data 
collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are
selected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the 
normalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. 
Limits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective 
field theory.
DOI: 10.17182/hepdata.79411.v1/t7
title: "Table 7" of "Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings"

description: Normalized differential W+W- cross section as a function of the angular separation between leptons. Both statistical and systematic uncertainties are included. Results are computed in a fiducial region defined by requiring zero jets at particle level with varying jet pT thresholds and requiring prompt leptons with pT &gt; 20 GeV and abs(eta) &lt; 2.5, before final-state radiation.
description: CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data 
collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are
selected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the 
normalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. 
Limits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective 
field theory.
DOI: 10.17182/hepdata.79411.v1/t8
title: "Table 8" of "Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings"

description: Measured cWWW/LAMBDA^2, cW/LAMBDA^2, and cB/LAMBDA^2 coupling constants.
description: CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data 
collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are
selected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the 
normalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. 
Limits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective 
field theory.