cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.54189.v1/t21
title: "Table 21" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t23
title: "Table 23" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t24
title: "Table 24" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t25
title: "Table 25" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t26
title: "Table 26" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t27
title: "Table 27" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t28
title: "Table 28" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t29
title: "Table 29" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t30
title: "Table 30" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.432 GeV**2, EPSILON=0.4478, W=1.192 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/t31
title: "Table 31" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.36 GeV**2, EPSILON=0.4458, W=1.232 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/t32
title: "Table 32" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.36 GeV**2, EPSILON=0.4458, W=1.232 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/t33
title: "Table 33" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.36 GeV**2, EPSILON=0.4458, W=1.232 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/t34
title: "Table 34" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.36 GeV**2, EPSILON=0.4458, W=1.232 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/t35
title: "Table 35" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.36 GeV**2, EPSILON=0.4458, W=1.232 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/t36
title: "Table 36" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.36 GeV**2, EPSILON=0.4458, W=1.232 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/t37
title: "Table 37" of "Neutral Pion Electroproduction in the Resonance Region at High $Q^2$"

description: Differential cross sections at Q**2=6.36 GeV**2, EPSILON=0.4458, W=1.232 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.