cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64353.v1/t8
title: "Table 8" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential dijet cross sections measured as a function of Q**2 and XI(2) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t9
title: "Table 9" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential trijet cross sections measured as a function of Q**2 and MEAN(PT(3JET)) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t12
title: "Table 12" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential normalised dijet cross sections measured as a function of Q**2 and MEAN(PT(2JET)) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t13
title: "Table 13" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential normalised inclusive dijet cross sections measured as a function of Q**2 and XI(2) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t14
title: "Table 14" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential normalised trijet cross sections measured as a function of Q**2 and MEAN(PT(3JET)) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t15
title: "Table 15" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential normalised trijet cross sections measured as a function of Q**2 and XI(3) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t16
title: "Table 16" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential normalised inclusive jet cross sections measured as a function of Q**2 and PT(JET) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.5% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t17
title: "Table 17" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential normalised dijet cross sections measured as a function of Q**2 and MEAN(PT(2JET)) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t18
title: "Table 18" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential normalised inclusive dijet cross sections measured as a function of Q**2 and XI(2) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).
DOI: 10.17182/hepdata.64353.v1/t19
title: "Table 19" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential normalised trijet cross sections measured as a function of Q**2 and MEAN(PT(3JET)) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.
description: DESY-HERA. Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 &lt; Q**2 &lt; 15000 GeV**2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. 

Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q**2 and the transverse momentum of the jet, PT(JET), and as a function of Q**2 and the proton longitudinal momentum fraction, XI, carried by the parton participating in the hard interaction. In addition normalised double differential jet cross sections are measured as the ratio of the jet cross sections to the inclusive neutral current cross sections in the respective Q**2 bins of the jet measurements. 

In dijet and trijet cross section measurements the variables used are labelled MEAN(PT(2JET)) and XI(2), and MEAN(PT(3JET)) and XI(3), respectively. These are defined as: 
 - MEAN(PT(2JET)) = (1/2) * ( PT(JET(1)) + PT(JET(2)) ). 
 - MEAN(PT(3JET)) = (1/3) * ( PT(JET(1)) + PT(JET(2)) + PT(JET(3)) ). 
 - XI(2) = X * ( 1 + (M(12)**2 / Q**2) ) where X is the Bjorken scaling variable and M(12) is the invariant mass of the two leading jets. 
 - XI(3) = X * ( 1 + (M(123)**2 / Q**2) ) where M(123) is the invariant mass of the three leading jets. 

Compared to earlier work, the measurements benefit from an improved reconstruction and calibration of the hadronic final state. The cross sections are compared to perturbative QCD calculations in next-to-leading order and are used to determine the running coupling and the value of the strong coupling constant as ALPHAS(M(Z)) = 0.1165 +- 0.0008 (exp) +- 0.0038 (pdf,theo).