cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.11120.v1/t81
title: "Table 81" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 275.0 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/t82
title: "Table 82" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 275.0 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/t83
title: "Table 83" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 275.0 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/t84
title: "Table 84" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 275.0 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/t85
title: "Table 85" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 305.0 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/t86
title: "Table 86" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino 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/t87
title: "Table 87" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino 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/t88
title: "Table 88" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino 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/t89
title: "Table 89" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino 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.