{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.180833.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2830401"}}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2026","description":"This paper presents a fully-corrected measurement of the energy-energy correlator (EEC) within jets in pp collisions. The EEC traces the energy flow as a highly energetic parton undergoes a QCD shower followed by the confinement of partons into hadrons, probing the correlation function of the energy flow inside jets. The EEC observable is measured as a function of the charged particle pair angular distance, $R_{\\mathrm{L}}$, for 20  $< p_{\\mathrm{T}}^{\\mathrm{ch\\; jet}}$ $<$ 80 $<$ $\\mathrm{GeV}/c$.In the perturbative region,(large $R_{\\mathrm{L}}$), a good agreement between the data and a next-to-leading-log perturbative QCD calculation is observed. In the non-perturbative region (small $R_{\\mathrm{L}}$), the data exhibits a linear $R_{\\mathrm{L}}$ dependence. There is a transition region in between, characterized by a turnover in the EEC distribution, corresponding to the confinement process. The peak of this transition region is located at $2.43 \\pm 0.14$ ${\\mathrm{GeV}/c}/\\langle p_{\\mathrm{T}}^{\\mathrm{ch\\; jet}}\\rangle$ for jets of various energies, indicating a common energy scale for the hadronization process. State-of-the-art Monte Carlo event generators are compared with the measurements, and can be used to constrain the parton shower and hadronization mechanisms.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.180833.v1/t1","@type":"Dataset","description":"Fully corrected $\\Sigma_{{EEC}}$ as a function of $R_{\\mathrm{L}}$ in the $p_{\\mathrm{T}}^{\\mathrm{ch\\; jet}}$ intervals 20-40, 40-60,and 60-80($\\mathrm{GeV}/c$).","name":"Figure 2"},{"@id":"https://doi.org/10.17182/hepdata.180833.v1/t2","@type":"Dataset","description":"Normalized $\\Sigma_{{EEC}}$ as a function of $\\langle p_T^{\\text{chJet}} \\rangle$$R_L$.","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.180833.v1/t3","@type":"Dataset","description":"Normalized $\\Sigma_{{EEC}}$ as a function of $\\langle p_T^{\\text{chJet}} \\rangle$$R_L$.","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.180833.v1/t4","@type":"Dataset","description":"Normalized $\\Sigma_{{EEC}}$ as a function of $\\langle p_T^{\\text{chJet}} \\rangle$$R_L$.","name":"Figure 3c"},{"@id":"https://doi.org/10.17182/hepdata.180833.v1/t5","@type":"Dataset","description":"Fully corrected $\\Sigma_{{EEC}}$ as a function of $R_{\\mathrm{L}}$ in the $p_{\\mathrm{T}}^{\\mathrm{ch\\; jet}}$ intervals 20-40, 40-60, and 60-80($\\mathrm{GeV}/c$) with $ p_T^{\\text{Track}}...","name":"Figure FigureC1_150MeV_threshold"},{"@id":"https://doi.org/10.17182/hepdata.180833.v1/t6","@type":"Dataset","description":"Fully corrected $\\Sigma_{{EEC}}$ as a function of $R_{\\mathrm{L}}$ in the $p_{\\mathrm{T}}^{\\mathrm{ch\\; jet}}$ intervals 20-40, 40-60, and 60-80($\\mathrm{GeV}/c$) with $ p_T^{\\text{Track}}...","name":"FigureC1_500MeV_threshold"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2830401?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/180833"}],"inLanguage":"en","name":"Exposing the parton-hadron transition within jets with energy-energy correlators in pp collisions at $\\sqrt{\\textit s}=5.02$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2830401?version=1","version":1}