{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.69212.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1380193"}},{"@id":"https://doi.org/10.1007/JHEP11(2015)127","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2015","description":"CERN-LHC.  We present a measurement of inclusive J/$\\psi$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\\rm T}$, in the backward ($-4.46 < y_{\\rm cms} < -2.96$) and forward ($2.03 < y_{\\rm cms} < 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 < y_{\\rm cms} < 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\\rm T}$-differential J/$\\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\\rm T}$ and $p^2_{\\rm T}$ values. The nuclear modification factor, $Q_{\\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\\rm T}$ for several centrality classes.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t1","@type":"Dataset","description":"Differential cross sections dsigma_JPsi/dydpt as function of pt at backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is statistical, the second...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t2","@type":"Dataset","description":"Differential cross sections d^2sigma^cent_JPsi/dydpt as function of pt for six centrality classes at forward (2.03<y_cms<3.53) centre-of-mass rapidity. The first uncertainty...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t3","@type":"Dataset","description":"Differential cross sections dsigma^cent_JPsi/dy for four centrality classes at mid-rapidity (-1.37<y_cms<0.43). The first uncertainty is statistical, the second and third...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t4","@type":"Dataset","description":"Differential cross sections dsigma^cent_JPsi/dy for six centrality classes at forward (2.03<y_cms<3.53) and backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t5","@type":"Dataset","description":"Nuclear modification factor Q_pA as function of centrality at forward (2.03<y_cms<3.53) and backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t6","@type":"Dataset","description":"Nuclear modification factor Q_pA as function of centrality in the mid-rapidity range (-1.37 <y_cms< 0.43). The first uncertainty is statistical,...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t7","@type":"Dataset","description":"Values of  and  for six centrality classes at forward (2.03<y_cms<3.53) and backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t8","@type":"Dataset","description":"Values of  and  at forward (2.03<y_cms<3.53) and backward (2.96<y_cms<4.46) centre-of-mass rapidity in pp collisions calculated based on an...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t9","@type":"Dataset","description":"Values of Delta as a function of centrality at forward (2.03<y_cms<3.53) and backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t10","@type":"Dataset","description":"Nuclear modification factor Q_pA as function of pT for six centrality classes at backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.69212.v1/t11","@type":"Dataset","description":"Nuclear modification factor Q_pA as a function of pT for six centrality classes at forward (2.03<y_cms<3.53) centre-of-mass rapidity. The first...","name":"Table 11"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1380193?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/69212"}],"inLanguage":"en","name":"Centrality dependence of inclusive J/$\\psi$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1380193?version=1","version":1}