{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77817.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1487727"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.05.060","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2017","description":"CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\\sqrt{s_{\\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\\rm AA}$ in the interval $3<~p_{\\rm T}<~ 18$ GeV/$c$. The $R_{\\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t1","@type":"Dataset","description":"Pb-Pb collision centrality 0-10%.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t2","@type":"Dataset","description":"Pb-Pb collision centrality 10-20%.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t3","@type":"Dataset","description":"Pb-Pb collision centrality 20-30%.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t4","@type":"Dataset","description":"Pb-Pb collision centrality 30-40%.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t5","@type":"Dataset","description":"Pb-Pb collision centrality 40-50%.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t6","@type":"Dataset","description":"Pb-Pb collision centrality 50-80%.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t7","@type":"Dataset","description":"Pb-Pb collision centrality 0-10%.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t8","@type":"Dataset","description":"Pb-Pb collision centrality 10-20%.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t9","@type":"Dataset","description":"Pb-Pb collision centrality 20-30%.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t10","@type":"Dataset","description":"Pb-Pb collision centrality 30-40%.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t11","@type":"Dataset","description":"Pb-Pb collision centrality 40-50%.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.77817.v1/t12","@type":"Dataset","description":"Pb-Pb collision centrality 50-80%.","name":"Table 12"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1487727?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/77817"}],"inLanguage":"en","name":"Measurement of the production of high-$p_{\\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\\mathbf{\\sqrt{\\it s_{\\rm{NN}}}}$ = 2.76 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1487727?version=1","version":1}