cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.11120.v1/t154
title: "Table 154" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.
description: Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (1) contains the F2 and xF3 distributions corrected to an isoscalar (iron) target. Parts 2 and 3 contain the differential cross sections themselves for neutrino an antineutrino beams respectively.. Numerical values of F2 and xF3 supplied by M. Tzanov.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (2) contains the neutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (3) contains the antineutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
DOI: 10.17182/hepdata.11120.v1/t155
title: "Table 155" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.
description: Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (1) contains the F2 and xF3 distributions corrected to an isoscalar (iron) target. Parts 2 and 3 contain the differential cross sections themselves for neutrino an antineutrino beams respectively.. Numerical values of F2 and xF3 supplied by M. Tzanov.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (2) contains the neutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (3) contains the antineutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
DOI: 10.17182/hepdata.11120.v1/t156
title: "Table 156" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.
description: Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (1) contains the F2 and xF3 distributions corrected to an isoscalar (iron) target. Parts 2 and 3 contain the differential cross sections themselves for neutrino an antineutrino beams respectively.. Numerical values of F2 and xF3 supplied by M. Tzanov.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (2) contains the neutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (3) contains the antineutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
DOI: 10.17182/hepdata.11120.v1/t157
title: "Table 157" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.
description: Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (1) contains the F2 and xF3 distributions corrected to an isoscalar (iron) target. Parts 2 and 3 contain the differential cross sections themselves for neutrino an antineutrino beams respectively.. Numerical values of F2 and xF3 supplied by M. Tzanov.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (2) contains the neutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (3) contains the antineutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
DOI: 10.17182/hepdata.11120.v1/t158
title: "Table 158" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.
description: Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (1) contains the F2 and xF3 distributions corrected to an isoscalar (iron) target. Parts 2 and 3 contain the differential cross sections themselves for neutrino an antineutrino beams respectively.. Numerical values of F2 and xF3 supplied by M. Tzanov.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (2) contains the neutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (3) contains the antineutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
DOI: 10.17182/hepdata.11120.v1/t159
title: "Table 159" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.
description: Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (1) contains the F2 and xF3 distributions corrected to an isoscalar (iron) target. Parts 2 and 3 contain the differential cross sections themselves for neutrino an antineutrino beams respectively.. Numerical values of F2 and xF3 supplied by M. Tzanov.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (2) contains the neutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
Fermilab Tevatron. Measurement of the differential cross sections for charged current neutrino and antineutrino interactions on iron, and the determination of the structure functions F2 and xF3 using a one-parameter fit to the inelasticity Y distributions. The data were collected during 1996-97 using separate high-purity neutrino and antineutrino beams with energies from 30 to 500 GeV.. This part (3) contains the antineutrino differential cross sections determined from the code downloaded from the NuTev web site & lt;a href=http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& gt; http://www-nutev.phyast.pitt.edu/results_2005/nutev_sf.html& lt;/a& gt; which also contains code for generating the point-to-point covariance matrix for detailed handling of errors.
DOI: 10.17182/hepdata.11124.v1/t1
title: "Table 1" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: The estimated systematic uncertainty is 6 PCT.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t2
title: "Table 2" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: The estimated systematic uncertainty is 6 PCT.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t3
title: "Table 3" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: The estimated systematic uncertainty is 6 PCT.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t4
title: "Table 4" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: Here THETA is the angle (in c.m. system) between the plane containing partons 1 and 3 and the plane containing partons 4 and 5: cos(theta) = [p1*p3]*[p4*p ]/(|[p1*p3]|*|[p4*p5]|). The estimated systematic uncertainty is 6 PCT.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t5
title: "Table 5" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: Here M is scaled invariant mass of jet pairs. The estimated systematic uncertainty is 6 PCT.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t6
title: "Table 6" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: Here M is scaled invariant mass of jet pairs. The estimated systematic uncertainty is 6 PCT.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t7
title: "Table 7" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: Here M is scaled invariant mass of jet pairs. The estimated systematic uncertainty is 6 PCT.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t8
title: "Table 8" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t9
title: "Table 9" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t10
title: "Table 10" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.
DOI: 10.17182/hepdata.11124.v1/t11
title: "Table 11" of "Studies of topological distributions of inclusive the three and four jet events in anti-P P collisions at s**(1/2) = 1800-GeV with the D0 detector"

description: The estimated systematic uncertainty is 6 PCT. 4-JET events in their center-of-mass system.
description: D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4 and 5 with E3 & gt; E4 & gt; E5.. In this part 3-JET events only.
D0 Collaboration. Studies of topological distributions of inclusive three- and four-jet events in P PBAR collisions at sqrt(s)=1800 GeV. Jets are labelled 3, 4, 5 and 6 with E3 & gt; E4 & gt; E5 & gt; E6.. In this part 4-JET events only.