{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.69247.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1384272"}},{"@id":"https://doi.org/10.1103/PhysRevC.92.044915","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2015","description":"The ATLAS Collaboration has measured the inclusive production of $Z$ bosons via their decays into electron and muon pairs in $p+$Pb collisions at $\\sqrt{s_{NN}}=5.02$ TeV at the Large Hadron Collider. The measurements are made using data corresponding to integrated luminosities of 29.4 nb$^{-1}$ and 28.1 nb$^{-1}$ for $Z \\rightarrow ee$ and $Z \\rightarrow \\mu\\mu$, respectively. The results from the two channels are consistent and combined to obtain a cross section times the $Z \\rightarrow \\ell\\ell$ branching ratio, integrated over the rapidity region $|y^{*}_{Z}|<3.5$, of 139.8 $\\pm$ 4.8 (stat.) $\\pm$ 6.2 (syst.) $\\pm$ 3.8 (lumi.) nb. Differential cross sections are presented as functions of the $Z$ boson rapidity and transverse momentum, and compared with models based on parton distributions both with and without nuclear corrections. The centrality dependence of $Z$ boson production in $p+$Pb collisions is measured and analyzed within the framework of a standard Glauber model and the model's extension for fluctuations of the underlying nucleon-nucleon scattering cross section.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.69247.v1/t1","@type":"Dataset","description":"The centrality bias factors derived from data as explained in the text. Model calculations shown in the Figure are found...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.69247.v1/t2","@type":"Dataset","description":"The differential $Z$ boson production cross section, $d\\sigma/dy^\\mathrm{*}_{Z}$, as a function of $Z$ boson rapidity in the center-of-mass frame $y^\\mathrm{*}_{Z}$,...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.69247.v1/t3","@type":"Dataset","description":"The differential cross section of $Z$ boson production multiplied by the Bjorken $x$ of the parton in the lead nucleus,...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.69247.v1/t4","@type":"Dataset","description":"The differential cross section of $Z$ boson production scaled by 1/$p_\\mathrm{T}^{Z}$, (1/$p_\\mathrm{T}^{Z}$) $d\\sigma /dp_\\mathrm{T}^{Z}$, for $-3<y^\\mathrm{*}_{Z}<2$.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.69247.v1/t5","@type":"Dataset","description":"The differential cross section of $Z$ boson production scaled by 1/$p_\\mathrm{T}^{Z}$, (1/$p_\\mathrm{T}^{Z}$) $d\\sigma /dp_\\mathrm{T}^{Z}$, for $-2<y^\\mathrm{*}_{Z}<0$ and $0<y^\\mathrm{*}_{Z}<2.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.69247.v1/t6","@type":"Dataset","description":"Centrality bias corrected $Z$ boson yields per event for $-3<y^\\mathrm{*}_{Z}<2$ scaled by by $\\langle N_{coll}\\rangle$. (To remove the centrality bias...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.69247.v1/t7","@type":"Dataset","description":"The rapidity differential Z boson yields per event scaled by $\\langle N_{coll}\\rangle$ for three centrality ranges.","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1384272?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/69247"}],"inLanguage":"en","name":"$Z$ boson production in $p+$Pb collisions at $\\sqrt{s_{NN}}=5.02$ TeV measured with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1384272?version=1","version":1}