{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.66344.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1321022"}},{"@id":"https://doi.org/10.1016/j.physletb.2014.11.041","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2014","description":"CERN-LHC.  We report on the production of inclusive $\\Upsilon(1S)$ and $\\Upsilon(2S)$ in p-Pb collisions at $\\sqrt{s_{NN}} = 5.02$ TeV at the LHC. \nThe measurement is performed with the ALICE detector at backward ($-4.46 < y_{{\\rm cms}} < -2.96$) and forward ($2.03 < y_{{\\rm cms}} < 3.53$) rapidity down to zero transverse momentum. The production cross section of the $\\Upsilon(1S)$ and $\\Upsilon(2S)$ are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of $\\Upsilon(1S)$. The data sets were taken in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.66344.v1/t1","@type":"Dataset","description":"Inclusive UPSI(1S) production cross section as a function of rapidity in p-Pb collisions at sqrt(s_NN) = 5.02 TeV. The data...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.66344.v1/t2","@type":"Dataset","description":"Inclusive UPSI(1S) production cross section as a function of rapidity in p-Pb collisions at sqrt(s_NN) = 5.02 TeV. The data...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.66344.v1/t3","@type":"Dataset","description":"Inclusive UPSI(2S) production cross section as a function of rapidity in p-Pb collisions at sqrt(s_NN) = 5.02 TeV. The data...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.66344.v1/t4","@type":"Dataset","description":"Nuclear modification factor of inclusive UPSI(1S) as a function of rapidity in p-Pb collisions at sqrt(s_NN) = 5.02 TeV. The...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.66344.v1/t5","@type":"Dataset","description":"Nuclear modification factor of inclusive UPSI(1S) as a function of rapidity in p-Pb collisions at sqrt(sNN) = 5.02 TeV. The...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.66344.v1/t6","@type":"Dataset","description":"Forward to backward ratio RFB of inclusive UPSI(1S) yields in p-Pb collisions at sqrt(sNN) = 5.02 TeV. The data was...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.66344.v1/t7","@type":"Dataset","description":"Ratios of the cross sections of UPSI(2S)->MU+MU- to UPSI(1S)->MU+MU- in p-Pb collisions at sqrt(sNN) = 5.02 TeV. The data was...","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1321022?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/66344"}],"inLanguage":"en","name":"Production of inclusive $\\Upsilon$(1S) and $\\Upsilon$(2S) in p-Pb collisions at $\\mathbf{\\sqrt{s_{{\\rm NN}}} = 5.02}$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1321022?version=1","version":1}