cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.54189.v1/t91
title: "Table 91" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.848 GeV**2, EPSILON=0.2251, W=1.152 GeV and COS(THETA(*))=0.5 for the large 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/t92
title: "Table 92" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.848 GeV**2, EPSILON=0.2251, W=1.152 GeV and COS(THETA(*))=0.83 for the large 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/t93
title: "Table 93" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.772 GeV**2, EPSILON=0.2236, W=1.192 GeV and COS(THETA(*))=-0.83 for the large 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/t101
title: "Table 101" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.692 GeV**2, EPSILON=0.2222, W=1.232 GeV and COS(THETA(*))=-0.17 for the large 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/t94
title: "Table 94" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.772 GeV**2, EPSILON=0.2236, W=1.192 GeV and COS(THETA(*))=-0.5 for the large 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/t95
title: "Table 95" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.772 GeV**2, EPSILON=0.2236, W=1.192 GeV and COS(THETA(*))=-0.17 for the large 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/t96
title: "Table 96" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.772 GeV**2, EPSILON=0.2236, W=1.192 GeV and COS(THETA(*))=0.17 for the large 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/t97
title: "Table 97" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.772 GeV**2, EPSILON=0.2236, W=1.192 GeV and COS(THETA(*))=0.5 for the large 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/t98
title: "Table 98" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.772 GeV**2, EPSILON=0.2236, W=1.192 GeV and COS(THETA(*))=0.83 for the large 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/t100
title: "Table 100" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.692 GeV**2, EPSILON=0.2222, W=1.232 GeV and COS(THETA(*))=-0.5 for the large 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/t102
title: "Table 102" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.692 GeV**2, EPSILON=0.2222, W=1.232 GeV and COS(THETA(*))=0.17 for the large 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/t103
title: "Table 103" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.692 GeV**2, EPSILON=0.2222, W=1.232 GeV and COS(THETA(*))=0.5 for the large 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/t104
title: "Table 104" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.692 GeV**2, EPSILON=0.2222, W=1.232 GeV and COS(THETA(*))=0.83 for the large 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/t105
title: "Table 105" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.608 GeV**2, EPSILON=0.2211, W=1.272 GeV and COS(THETA(*))=-0.83 for the large 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/t106
title: "Table 106" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.608 GeV**2, EPSILON=0.2211, W=1.272 GeV and COS(THETA(*))=-0.5 for the large 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/t99
title: "Table 99" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=7.692 GeV**2, EPSILON=0.2222, W=1.232 GeV and COS(THETA(*))=-0.83 for the large 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.