cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.11120.v1/t27
title: "Table 27" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 35.0 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/t28
title: "Table 28" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 35.0 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/t29
title: "Table 29" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 45.0 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/t30
title: "Table 30" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 45.0 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/t31
title: "Table 31" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 45.0 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/t32
title: "Table 32" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Differential cross sections at neutrino energy 45.0 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/t33
title: "Table 33" 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 0.015, 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/t34
title: "Table 34" 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 0.125, 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/t35
title: "Table 35" 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 0.275, 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.