cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64267.v1/t4
title: "Table 4" of "Cross Section and Transverse Single-Spin Asymmetry of $\eta$ Mesons in $p^{\uparrow}+p$ Collisions at $\sqrt{s}=200$ GeV at Forward Rapidity"

description: ASYM for ETA mesons measured as a function of PT for ABS(XF) &gt; 0.2. Uncertainties listed are those due to the statistics, the PT uncorrelated uncertainties due to extracting ASYM, and the correlated relative luminosity uncertainty.
description: BNL-RHIC. We present a measurement of the cross section and transverse single-spin asymmetry ASYM for ETA mesons at forward pseudorapidity (3.0 &lt; ABS(ETARAP) &lt; 3.8). The data used in this analysis is from P(UP) P collisions at sqrt(s) = 200 GeV during the 2008 data taking period at RHIC. A total integrated luminosity of 6.65 pb^{-1} was sampled for these results. 

The invariant cross section of ETA mesons as a function of transverse momentum, PT, is presented. The asymmetry of the peak region, ASYM(PEAK), and the asymmetry of the background regions, ASYM(BG), measured as functions of XF from a high-PT triggered (the 4X4B triggered) dataset are presented. The asymmetries ASYM have been measured as a function of Feynman-x, XF, in the range 0.2 &lt; ABS(XF) &lt; 0.7 as well as a function of transverse momentum in the range 1.0 &lt; PT &lt; 4.5 GeV. The asymmetry averaged over positive XF is MEAN(ASYM) = 0.061 +- 0.014.
DOI: 10.17182/hepdata.64353.v1/t1
title: "Table 1" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential inclusive jet cross sections measured as a function of Q**2 and PT(JET) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.5% 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/t2
title: "Table 2" 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 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/t3
title: "Table 3" 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 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/t4
title: "Table 4" 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 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/t10
title: "Table 10" 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 XI(3) 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/t11
title: "Table 11" 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 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/t5
title: "Table 5" 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 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/t6
title: "Table 6" of "Measurement of Multijet Production in ep Collisions at High Q^2 and Determination of the Strong Coupling alpha_s"

description: Double-differential 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/t7
title: "Table 7" 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 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).