{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.113760.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1829411"}},{"@id":"https://doi.org/10.1007/JHEP09(2021)211","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2022","description":"CERN-LHC. Jet fragmentation transverse momentum ($j_\\mathrm{T}$) distributions are measured in proton-proton (pp) and proton-lead (p--Pb) collisions at $\\sqrt{s_\\mathrm{NN}}$ with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-$k_\\mathrm{T}$ algorithm with resolution parameter $R = 0.4$ in the pseudorapidity range $|\\eta|<0.25$. The $j_\\mathrm{T}$ values are calculated for charged particles inside a fixed cone with a radius $R = 0.4$ around the reconstructed jet axis. The $j_\\mathrm{T}$ distributions are further characterised by fitting them with a function composed of an inverse gamma function for higher $j_\\mathrm{T}$ values (called the wide component), related to the perturbative component of the fragmentation process, and with a Gaussian for lower $j_\\mathrm{T}$ values (called the narrow component), predominantly connected to the hadronisation process.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.113760.v1/t1","@type":"Dataset","description":"$j_\\mathrm{T}$ distribution in pp collisions at $\\sqrt{s}$ = 5.02 TeV in $40 < p_\\mathrm{T, jet}$ < 60 GeV/$c$.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.113760.v1/t2","@type":"Dataset","description":"$j_\\mathrm{T}$ distributions in p--Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV in $40 < p_\\mathrm{T, jet}$ < 150 GeV/$c$.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.113760.v1/t3","@type":"Dataset","description":"$\\sqrt{\\langle j_\\mathrm{T}^2 \\rangle }$ values for the narrow and wide components in pp collisions at $\\sqrt{s}$ = 5.02 TeV in...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.113760.v1/t4","@type":"Dataset","description":"$\\sqrt{\\langle j_\\mathrm{T}^2 \\rangle }$ values for the narrow and wide components in p--Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV in...","name":"Table 4"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1829411?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/113760"}],"inLanguage":"en","name":"Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1829411?version=1","version":1}