cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.11120.v1/t36
title: "Table 36" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 55.0 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/t37
title: "Table 37" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 65.0 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/t38
title: "Table 38" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 65.0 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/t39
title: "Table 39" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 65.0 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/t40
title: "Table 40" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 65.0 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/t41
title: "Table 41" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 75.0 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/t42
title: "Table 42" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 75.0 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/t43
title: "Table 43" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 75.0 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/t44
title: "Table 44" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 75.0 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.