{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.64754.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1278730"}},{"@id":"https://doi.org/10.1016/j.nuclphysb.2014.07.019","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"COMPASS Collaboration"},"creator":{"@type":"Organization","name":"COMPASS Collaboration"},"datePublished":"2019","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.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t1","@type":"Dataset","description":"ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical and systematic.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t2","@type":"Dataset","description":"ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical and systematic.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t3","@type":"Dataset","description":"ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical and systematic.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t4","@type":"Dataset","description":"ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical and systematic.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t5","@type":"Dataset","description":"ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical and systematic.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t6","@type":"Dataset","description":"ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical and systematic.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t7","@type":"Dataset","description":"ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical and systematic.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t8","@type":"Dataset","description":"ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical and systematic.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t9","@type":"Dataset","description":"ASYMUU(COS(2*PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical and systematic.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t10","@type":"Dataset","description":"ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the first XB bin. The errors are statistical and systematic.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t11","@type":"Dataset","description":"ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the second XB bin. The errors are statistical and systematic.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t12","@type":"Dataset","description":"ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the third XB bin. The errors are statistical and systematic.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t13","@type":"Dataset","description":"ASYMUU(COS(PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the last XB bin. The errors are statistical and systematic.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t14","@type":"Dataset","description":"ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the first XB bin. The errors are statistical and systematic.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t15","@type":"Dataset","description":"ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the second XB bin. The errors are statistical and systematic.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t16","@type":"Dataset","description":"ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the third XB bin. The errors are statistical and systematic.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.64754.v2/t17","@type":"Dataset","description":"ASYMUU(COS(2*PHI(HADRON))) 3d asymmetries for positive and negative hadrons in the last XB bin. The errors are statistical and systematic.","name":"Table 17"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1278730?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/64754"}],"inLanguage":"en","name":"Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1278730?version=2","version":2}