cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.11116.v1/t80
title: "Table 80" of "Measurement of e p --&gt; e' p pi+ pi- and baryon resonance analysis."

description: Measured c.m. angular distribution of the PI- for the W range 1975 to 2000GeV.
description: Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the PI+_PI-, (P=4_5) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the P_PI, (P=4_6) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the angular distribution of the PI-, (P=5).
DOI: 10.17182/hepdata.11116.v1/t81
title: "Table 81" of "Measurement of e p --&gt; e' p pi+ pi- and baryon resonance analysis."

description: Measured c.m. angular distribution of the PI- for the W range 2000 to 2025GeV.
description: Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the PI+_PI-, (P=4_5) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the P_PI, (P=4_6) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the angular distribution of the PI-, (P=5).
DOI: 10.17182/hepdata.11116.v1/t82
title: "Table 82" of "Measurement of e p --&gt; e' p pi+ pi- and baryon resonance analysis."

description: Measured c.m. angular distribution of the PI- for the W range 2025 to 2050GeV.
description: Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the PI+_PI-, (P=4_5) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the P_PI, (P=4_6) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the angular distribution of the PI-, (P=5).
DOI: 10.17182/hepdata.11116.v1/t83
title: "Table 83" of "Measurement of e p --&gt; e' p pi+ pi- and baryon resonance analysis."

description: Measured c.m. angular distribution of the PI- for the W range 2050 to 2075GeV.
description: Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the PI+_PI-, (P=4_5) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the P_PI, (P=4_6) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the angular distribution of the PI-, (P=5).
DOI: 10.17182/hepdata.11116.v1/t84
title: "Table 84" of "Measurement of e p --&gt; e' p pi+ pi- and baryon resonance analysis."

description: Measured c.m. angular distribution of the PI- for the W range 2075 to 2100GeV.
description: Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the PI+_PI-, (P=4_5) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the cross sections w.r.t. the P_PI, (P=4_6) mass.
Jefferson Lab. Measurement of the cross sections for the reaction E P --& gt; E P PI+ PI- in the resonance region for W from 1.4 to 2.1 Gev and Q**2 from 0.5 to 1.5 GeV**2. The data were taken with the CLAS spectrometer with an electron beam energy of 2.567 GeV for the lower two Q**2 ranges and 4.247 for the higher Q**2 range. Numerical values supplied by Marco Ripani.. This part gives the angular distribution of the PI-, (P=5).
DOI: 10.17182/hepdata.11117.v1/t1
title: "Table 1" of "Yield of $\mu^- e^+$ Pairs in Muon-neutrino $N$ Interaction in Skat Bubble Chamber"

description: No description provided.
description: THE PARAMETERS OF THE 6 MU- E+ EVENTS WITH ENERGY(E+) & gt; 400 MEV ARE LISTED IN THE TABLE 2 (NOT ENCODED).
DOI: 10.17182/hepdata.11117.v1/t2
title: "Table 2" of "Yield of $\mu^- e^+$ Pairs in Muon-neutrino $N$ Interaction in Skat Bubble Chamber"

description: No description provided.
description: THE PARAMETERS OF THE 6 MU- E+ EVENTS WITH ENERGY(E+) & gt; 400 MEV ARE LISTED IN THE TABLE 2 (NOT ENCODED).
DOI: 10.17182/hepdata.11120.v1/t1
title: "Table 1" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Measurement of F2 at X = 0.015.
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/t2
title: "Table 2" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Measurement of F2 at X = 0.045.
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/t3
title: "Table 3" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Measurement of F2 at X = 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/t4
title: "Table 4" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Measurement of F2 at X = 0.125.
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/t5
title: "Table 5" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Measurement of F2 at X = 0.175.
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/t6
title: "Table 6" of "Precise measurement of neutrino and anti-neutrino differential cross sections."

description: Measurement of F2 at X = 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.