cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.78261.v1/t15
title: "Table 15" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t16
title: "Table 16" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t17
title: "Table 17" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t18
title: "Table 18" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t19
title: "Table 19" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t21
title: "Table 21" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t20
title: "Table 20" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t22
title: "Table 22" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t23
title: "Table 23" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t24
title: "Table 24" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t25
title: "Table 25" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t26
title: "Table 26" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t27
title: "Table 27" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t29
title: "Table 29" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t28
title: "Table 28" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t30
title: "Table 30" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t31
title: "Table 31" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t32
title: "Table 32" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t33
title: "Table 33" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t34
title: "Table 34" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t35
title: "Table 35" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t36
title: "Table 36" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t37
title: "Table 37" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t38
title: "Table 38" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t39
title: "Table 39" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t40
title: "Table 40" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.