{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.95539.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1762360"}},{"@id":"https://doi.org/10.1016/j.physletb.2020.135486","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2020","description":"CERN-LHC-ALICE. $\\Upsilon$ production in $\\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\\sqrt{s_{_{\\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03<y_{\\rm{cms}}<3.53$ and $-4.46<y_{\\rm{cms}}<-2.96$, down to zero transverse momentum. In this work, results on the $\\Upsilon$(1S) production cross section as a function of rapidity and transverse momentum are presented. The corresponding nuclear modification factor shows a suppression of the $\\Upsilon$(1S) yields with respect to \\mbox{pp} collisions, both at forward and backward rapidity. This suppression is stronger in the low transverse momentum region and shows no significant dependence on the centrality of the interactions. Furthermore, the $\\Upsilon$(2S) nuclear modification factor is evaluated, suggesting a suppression similar to that of the $\\Upsilon$(1S). A first measurement of the $\\Upsilon$(3S) has also been performed. Finally, results are compared with previous ALICE measurements in $\\mbox{p--Pb}$ collisions at $\\sqrt{s_{_{\\rm {NN}}}} = 8.16$~TeV and with theoretical calculations.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t1","@type":"Dataset","description":"$\\Upsilon$(1S) differential cross section as a function of $y_{\\rm cms}$, in p--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t2","@type":"Dataset","description":"$\\Upsilon$(2S) differential cross section times as a function of $y_{\\rm cms}$, in p--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV....","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t3","@type":"Dataset","description":"$\\Upsilon$(3S) differential cross section as a function of $y_{\\rm cms}$, in p--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t4","@type":"Dataset","description":"$\\Upsilon$(1S) differential cross section as a function of $p_{\\rm T}$, at forward rapidity at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV .The...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t5","@type":"Dataset","description":"$\\Upsilon$(1S) differential cross section as a function of $p_{\\rm T}$, at backward rapidity at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV .The...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t6","@type":"Dataset","description":"Ratio of $\\Upsilon$(2S) over $\\Upsilon$(1S) yields in p--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical,...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t7","@type":"Dataset","description":"Ratio of $\\Upsilon$(3S) over $\\Upsilon$(1S) yields in p--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical,...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t8","@type":"Dataset","description":"$\\Upsilon$(1S) $R_{\\rm pPb}$ values at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t9","@type":"Dataset","description":"$\\Upsilon$(1S) $R_{\\rm pPb}$ as a function of $y_{\\rm {cms}}$ at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical,...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t10","@type":"Dataset","description":"$\\Upsilon$(1S) $R_{\\rm pPb}$ as a function of $p_{\\rm T}$ at backward rapidity at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t11","@type":"Dataset","description":"$\\Upsilon$(1S) $R_{\\rm pPb}$ as a function of $p_{\\rm T}$ at forward rapidity at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t12","@type":"Dataset","description":"$\\Upsilon$(1S) $Q_{\\rm pPb}$ as a function of $$ at backward rapidity at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t13","@type":"Dataset","description":"$\\Upsilon$(1S) $Q_{\\rm pPb}$ as a function of $$ at forward rapidity at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t14","@type":"Dataset","description":"$\\Upsilon$(1S) $R_{\\rm pPb}$ values at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t15","@type":"Dataset","description":"$\\Upsilon$(2S) $R_{\\rm pPb}$ values at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t16","@type":"Dataset","description":"$\\Upsilon$(3S) $R_{\\rm pPb}$ values at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t17","@type":"Dataset","description":"Ratio of $\\Upsilon$(2S) to $\\Upsilon$(1S) $R_{\\rm pPb}$ at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV as a function of $y_{\\rm cms}$ .The...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.95539.v1/t18","@type":"Dataset","description":"Ratio of $\\Upsilon$(3S) to $\\Upsilon$(1S) $R_{\\rm pPb}$ at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV as a function of $y_{\\rm cms}$ .The...","name":"Table 18"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1762360?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/95539"}],"inLanguage":"en","name":"Inclusive $\\Upsilon$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1762360?version=1","version":1}