{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.78374.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1501480"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.03.018","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"COMPASS Collaboration"},"creator":{"@type":"Organization","name":"COMPASS Collaboration"},"datePublished":"2017","description":"Final results from the inclusive measurement of deep-inelastic polarised-muon scattering on longitudinally polarised deuterons using a ${^6}$LiD target. The data were taken at 160\u2009GeV beam energy and the results are shown for the kinematic range $1\\,($GeV$/c)^2<Q^2<100\\,($GeV$/c)^2$ in photon virtuality, $0.004<x<0.7$ in the Bjorken scaling variable and $W>4\\,$GeV$/c^2$ in the mass of the hadronic final state. The deuteron double-spin asymmetry $A_1^d$ and the deuteron longitudinal-spin structure function $g_1^d$ are presented in bins of $x$ and $Q^2$. The updated results on the non-singlet spin structure function $g_1^{NS} = g_1^p-g_1^n$ using the final deuteron results are also given. The parameters of the QCD fit described in a previous paper are given using the updated deuteron data.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.78374.v1/t1","@type":"Dataset","description":"Values of $A_1^d$ and $g_1^d$ for the COMPASS deuteron data at 160 GeV in $x$ bins averaged over $Q^2$.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.78374.v1/t2","@type":"Dataset","description":"Values of $A_1^d$ and $g_1^d$ for the COMPASS deuteron data at 160 GeV in (x, $Q^2$) bins.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.78374.v1/t3","@type":"Dataset","description":"Values of $g_1^{NS}$ for the COMPASS data in $x$ bins averaged over $Q^2$.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.78374.v1/t4","@type":"Dataset","description":"Values of $g_1^{NS}$ for the COMPASS data in ($x$, $Q^2$) bins.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.78374.v1/t5","@type":"Dataset","description":"Parameters of two solutions of the QCD fit. The assumed functional form at $Q^2_0 = 1 ($GeV$/c)^2$ is $q(x) =...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.78374.v1/t6","@type":"Dataset","description":"Normalisations of the different data sets used in the QCD fit.","name":"Table 6"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1501480?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/78374"}],"inLanguage":"en","name":"Final COMPASS results on the deuteron spin-dependent structure function $g_1^{\\rm d}$ and the Bjorken sum rule","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1501480?version=1","version":1}