{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.70846.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1355544"}},{"@id":"https://doi.org/10.1007/JHEP06(2015)055","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2016","description":"CERN-LHC.  Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\\psi$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\\rm cms}$) regions, down to zero $p_{\\rm T}$. The measurements are performed at forward (2.03<$y_{\\rm cms}$<3.53), mid (-1.37<$y_{\\rm cms}$<0.43) and backward (-4.46<$y_{\\rm cms}$<-2.96) centre of mass rapidities.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t1","@type":"Dataset","description":"$p_{\\rm T}$-differential inclusive cross section ${\\rm d}^2\\sigma^{J/\\psi}/{\\rm d}y{\\rm d}p_{T}$ in the backward rapidity range (-4.46<$y_{\\rm cms}$<-2.96). The first uncertainty is...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t2","@type":"Dataset","description":"$p_{\\rm T}$-differential inclusive cross section ${\\rm d}^2\\sigma^{J/\\psi}/{\\rm d}y{\\rm d}p_{T}$ in the mid-rapidity range (-1.37<$y_{\\rm cms}$<0.43). The first uncertainty is statistical,...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t3","@type":"Dataset","description":"$p_{\\rm T}$-differential inclusive cross section ${\\rm d}^2\\sigma^{J/\\psi}/{\\rm d}y{\\rm d}p_{T}$ in the forward rapidity range (2.03<$y_{\\rm cms}$<3.53). The first uncertainty is...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t4","@type":"Dataset","description":"$p_{\\rm T}$ dependence of the J/$\\psi$ nuclear modification factor $R_{\\rm pA}$ in the backward rapidity range (-4.46<$y_{\\rm cms}$<-2.96). The first...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t5","@type":"Dataset","description":"$p_{\\rm T}$ dependence of the J/$\\psi$ nuclear modification factor $R_{\\rm pA}$ in the mid-rapidity range (-1.37<$y_{\\rm cms}$<-0.43). The first uncertainty...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t6","@type":"Dataset","description":"$p_{\\rm T}$ dependence of the J/$\\psi$ nuclear modification factor $R_{\\rm pA}$ in the forward rapidity range (2.03<$y_{\\rm cms}$<3.53). The first...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t7","@type":"Dataset","description":"Estimate of the $p_{\\rm T}$-dependence of the Cold Nuclear Matter effects in Pb-Pb collisions calculated as $R^2_{\\rm pPb}$. The first...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t8","@type":"Dataset","description":"Estimate of the $p_{\\rm T}$-dependence of the Cold Nuclear Matter effects in Pb-Pb collisions calculated as $R_{\\rm pPb}$(-4.46 <y< -2.96)...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.70846.v1/t9","@type":"Dataset","description":"$p_{\\rm T}$-dependence of the ratio between the $R_{\\rm PbPb}$ and the cold nuclear matter effects evaluated as $R_{\\rm pPb}$(-4.46 <y<...","name":"Table 9"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1355544?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/70846"}],"inLanguage":"en","name":"Rapidity and transverse-momentum dependence of the inclusive J/$\\mathbf{\\psi}$ nuclear modification factor in p-Pb collisions at $\\mathbf{\\sqrt{\\textit{s}_{NN}}}=5.02$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1355544?version=1","version":1}