cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.54189.v1/t59
title: "Table 59" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.212 GeV**2, EPSILON=0.4411, W=1.312 GeV and COS(THETA(*))=0.7 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t60
title: "Table 60" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.212 GeV**2, EPSILON=0.4411, W=1.312 GeV and COS(THETA(*))=0.9 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t61
title: "Table 61" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=-0.9 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t62
title: "Table 62" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=-0.7 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t63
title: "Table 63" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=-0.5 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t64
title: "Table 64" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=-0.3 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t65
title: "Table 65" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=-0.1 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t66
title: "Table 66" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=0.1 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t67
title: "Table 67" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=0.3 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t68
title: "Table 68" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=0.5 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t69
title: "Table 69" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=0.7 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t70
title: "Table 70" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.136 GeV**2, EPSILON=0.4383, W=1.352 GeV and COS(THETA(*))=0.9 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t72
title: "Table 72" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.06 GeV**2, EPSILON=0.4351, W=1.392 GeV and COS(THETA(*))=-0.7 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t71
title: "Table 71" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.06 GeV**2, EPSILON=0.4351, W=1.392 GeV and COS(THETA(*))=-0.9 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t73
title: "Table 73" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.06 GeV**2, EPSILON=0.4351, W=1.392 GeV and COS(THETA(*))=-0.5 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
DOI: 10.17182/hepdata.54189.v1/t74
title: "Table 74" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.06 GeV**2, EPSILON=0.4351, W=1.392 GeV and COS(THETA(*))=-0.3 for the small SOS spectrometer.
description: Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.
Jefferson Lab.-Hall C. Measurement of the differential cross sections for neutral pion electroproduction in the process E- P --& gt; E- PI0 P at Q**2 from 6.06 to 7.924 GeV**2. The experiment uses two spectrometers. The HMS and SOS in Hall C with an unpolarized electron beam of around 5.5 GeV hitting at liquid hydrogen target. The data were gathered in the 2003 run period. Data are given for two settings of the SOS (Short Orbital Spectrometer).. The first DSYS error is due to the uncertainty in the normalization. The second is the remainder of the systematic uncertainty.