cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64754.v2/t6
title: "Table 6" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t7
title: "Table 7" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t8
title: "Table 8" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t9
title: "Table 9" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t10
title: "Table 10" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the first XB bin. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t11
title: "Table 11" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the second XB bin. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t12
title: "Table 12" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the third XB bin. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t13
title: "Table 13" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the last XB bin. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t1
title: "Table 1" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t2
title: "Table 2" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t14
title: "Table 14" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the first XB bin. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t15
title: "Table 15" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the second XB bin. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t16
title: "Table 16" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the third XB bin. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t17
title: "Table 17" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the last XB bin. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t3
title: "Table 3" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t4
title: "Table 4" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t5
title: "Table 5" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t8
title: "Table 8" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t10
title: "Table 10" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the first XB bin. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t11
title: "Table 11" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the second XB bin. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t12
title: "Table 12" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the third XB bin. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t6
title: "Table 6" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t7
title: "Table 7" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t9
title: "Table 9" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t13
title: "Table 13" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the last XB bin. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v1/t14
title: "Table 14" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the first XB bin. The errors are statistical only.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.