{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.11211.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/726689"}},{"@id":"https://doi.org/10.1103/PhysRevD.75.012007","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"HERMES Collaboration"},"creator":{"@type":"Organization","name":"HERMES Collaboration"},"datePublished":"2006","description":"DESY-HERA. Precise measurements of the spin structure functions and virtual photon asymmetries of the proton and deuteron over the kinematic range in X from 0.0041 to 0.9 and in Q**2 from 0.18 to 20 GeV**2. The data were collected in DIS of 27.6 GeV longitudinally polarized positrons from longitudinally polarized hydrogen and deuterium gas targets internal to the HERA ring. The neutron structure function is extracted by combining the proton and deuteron data.. This part (1) contains the structure function and asymmetry measurements (part 2 contains the correlation matrices).\nDESY-HERA. Precise measurements of the spin structure functions and virtual photon asymmetries of the proton and deuteron over the kinematic range in X from 0.0041 to 0.9 and in Q**2 from 0.18 to 20 GeV**2. The data were collected in DIS of 27.6 GeV longitudinally polarized positrons from longitudinally polarized hydrogen and deuterium gas targets internal to the HERA ring. The neutron structure function is extracted by combining the proton and deuteron data.. This part (2) contains the correlation matrices. (part 1 contains the structure functions and asymmetry measurements).","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t1","@type":"Dataset","description":"Integrals of G1 for P, DEUT and N targets.. The second DSYS systematic error is due to the uncertainty in...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t2","@type":"Dataset","description":"Integrals of G1 for the Non-Singlet contributions.. The second DSYS systematic error is due to the uncertainty in the parameterizations...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t3","@type":"Dataset","description":"Integrals of G1 over different X ranges for P target at various Q*2 values. The second DSYS systematic error is...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t4","@type":"Dataset","description":"Integrals of G1 over different X ranges for DEUT target at various Q*2 values. The second DSYS systematic error is...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t5","@type":"Dataset","description":"Integrals of G1 over different X ranges for N target at various Q*2 values. The second DSYS systematic error is...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t6","@type":"Dataset","description":"Integral of G1 for the Non-Singet contribution. The second DSYS systematic error is due to the uncertainty in the parameterizations...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t7","@type":"Dataset","description":"The measured and Born asymmetries for the proton target at the average values of the average values of X, Y,and...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t8","@type":"Dataset","description":"The measured and Born asymmetries for the deuterium target at the average values of the average values of X, Y,and...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t9","@type":"Dataset","description":"Virtual photon asymmetries A1 for the proton and deuterium targets at the average values of X,and Q**2 in 45 bins....","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t10","@type":"Dataset","description":"Structure functions G1 for the proton and deuterium targets at the average values of X,and Q**2 in 45 bins. The...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t11","@type":"Dataset","description":"Virtual photon asymmetries A1 for the proton and deuterium targets at the average values of X,and Q**2 in 19 bins....","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t12","@type":"Dataset","description":"Structure functions G1 for the proton and deuterium targets at the average values of X,and Q**2 in 19 bins. The...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t13","@type":"Dataset","description":"Structure functions G1 for the proton and deuterium targets at the average values of X,and Q**2 in 15 bins. The...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t14","@type":"Dataset","description":"Virtual photon asymmetries A1 for the proton and deuterium targets at the average values of X,and Q**2 in 15 bins....","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t15","@type":"Dataset","description":"Structure functions G1(n) and G1(NS)for the proton and deuterium targets at the average values of X,and Q**2 in 45 bins....","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t16","@type":"Dataset","description":"Structure functions G1(n) and G1(NS)for the proton and deuterium targets at the average values of X,and Q**2 in 19 bins....","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t17","@type":"Dataset","description":"Structure functions G1(n) and G1(NS)for the proton and deuterium targets at the average values of X,and Q**2 in 15 bins....","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t18","@type":"Dataset","description":"Correlation matrix for the Asymmetry, A1 and G1 for the P target at the average values of X and Q**2...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t19","@type":"Dataset","description":"Correlation matrix for the Asymmetry, A1 and G1 for the DEUT target at the average values of X and Q**2...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t20","@type":"Dataset","description":"Correlation matrix for G1 for the P target in 19 X bins (averaged over Q**2).","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t21","@type":"Dataset","description":"Correlation matrix for G1 for the DEUT target in 19 X bins (averaged over Q**2).","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t22","@type":"Dataset","description":"Correlation matrix for G1 for the P target in 15 X bins (Q**2 > 1 GeV**2), averaged over Q**2.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.11211.v1/t23","@type":"Dataset","description":"Correlation matrix for G1 for the DEUT target in 15 X bins (Q**2 > 1 GeV**2), averaged over Q**2.","name":"Table 23"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins726689?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/11211"}],"inLanguage":"en","name":"Precise determination of the spin structure function g(1) of the proton, deuteron and neutron.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins726689?version=1","version":1}