{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.142624.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2648614"}},{"@id":"https://doi.org/10.1007/JHEP08(2023)006","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2023","description":"Measurements of the production of electrons from heavy-flavour hadron decays in pp collisions at $\\sqrt{s} = 13$ TeV at midrapidity with the ALICE detector are presented down to a transverse momentum ($p_{\\rm T}$) of 0.2 GeV$/c$ and up to $p_{\\rm T} = 35$ GeV$/c$, which is the largest momentum range probed for inclusive electron measurements in ALICE. In p$-$Pb collisions, the production cross section and the nuclear modification factor of electrons from heavy-flavour hadron decays are measured in the $p_{\\rm T}$ range $0.5 < p_{\\rm T} < 26$ GeV$/c$ at $\\sqrt{s_{\\rm NN}} = 8.16$ TeV. The nuclear modification factor is found to be consistent with unity within the statistical and systematic uncertainties. In both collision systems, first measurements of the yields of electrons from heavy-flavour hadron decays in different multiplicity intervals normalised to the multiplicity-integrated yield (self-normalised yield) at midrapidity are reported as a function of the self-normalised charged-particle multiplicity estimated at midrapidity. The self-normalised yields in pp and p$-$Pb collisions grow faster than linear with the self-normalised multiplicity. A strong $p_{\\rm T}$ dependence is observed in pp collisions, where the yield of high-$p_{\\rm T}$ electrons increases faster as a function of multiplicity than the one of low-$p_{\\rm T}$ electrons. The measurement in p$-$Pb collisions shows no $p_{\\rm T}$ dependence within uncertainties. The self-normalised yields in pp and p$-$Pb collisions are compared with measurements of other heavy-flavour, light-flavour, and strange particles, and with Monte Carlo simulations.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.142624.v1/t1","@type":"Dataset","description":"pT-differential cross section of electrons from heavy-flavour hadron decays in pp collisions at $\\sqrt{s}$ = 13 TeV measured at midrapidity","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.142624.v1/t2","@type":"Dataset","description":"pT-differential cross section of electrons from heavy-flavour hadron decays in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV measured at...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.142624.v1/t3","@type":"Dataset","description":"The Nuclear modification factor RpPb of electrons from heavy-flavour hadron decays in p--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.142624.v1/t4","@type":"Dataset","description":"Self-normalised yield of electrons from heavy-flavour hadron decays as a function of normalised charged-particle pseudorapidity density at midrapidity computed in...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.142624.v1/t5","@type":"Dataset","description":"Self-normalised yield of electrons from heavy-flavour hadron decays as a function of normalised charged-particle pseudorapidity density at midrapidity computed in...","name":"Table 5"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2648614?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/142624"}],"inLanguage":"en","name":"Inclusive and multiplicity dependent production of electrons from heavy-flavour hadron decays in pp and p$-$Pb collisions","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2648614?version=1","version":1}