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Statistical (bars) and systematic and extrapolation (brackets) uncertainties are shown. The measurements are compared with calculations from the theoretical models nCTEQ15~\\cite{Kusina:2017gkz,Kusina:2020dki,Kovarik:2015cma} and EPPS16~\\cite{Eskola:2016oht} that include only initial-state effects. The uncertainty bands on the models represent the 90\\% confidence level.","filename":"Integrated_Raa.png","material":"preprint"},{"key":"c1f23a3f36d308409a3399172b82a61d","url":"https://inspirehep.net/files/c1f23a3f36d308409a3399172b82a61d","label":"fig:LcDWithModels","source":"arxiv","caption":"Left: \\LcD ratio in pp and \\pPb collisions as a function of \\pt, compared with the QCM model~\\cite{Li:2017zuj,Li:2021nhq}. Right: \\LcD ratio as a function of \\pt in pp collisions at \\sqrtsfive, including comparisons with models~\\cite{He:2019tik,Christiansen:2015yqa,Skands:2014pea,Minissale:2020bif,Li:2021nhq}","filename":"LcDppVspPb_5TeV-lowpT.png","material":"preprint"},{"key":"ae841bb5d8bcbe8aab0676e8b5a08f2c","url":"https://inspirehep.net/files/ae841bb5d8bcbe8aab0676e8b5a08f2c","label":"fig:LcDWithModels","source":"arxiv","caption":"Left: \\LcD ratio in pp and \\pPb collisions as a function of \\pt, compared with the QCM model~\\cite{Li:2017zuj,Li:2021nhq}. Right: \\LcD ratio as a function of \\pt in pp collisions at \\sqrtsfive, including comparisons with models~\\cite{He:2019tik,Christiansen:2015yqa,Skands:2014pea,Minissale:2020bif,Li:2021nhq}","filename":"LcDpp5vsModels-lowpT.png","material":"preprint"}],"license":[{"url":"https://creativecommons.org/licenses/by/4.0/","license":"CC BY 4.0","material":"publication"},{"url":"http://creativecommons.org/licenses/by/4.0/","license":"CC BY 4.0","material":"preprint"}],"texkeys":["ALICE:2022exq","ALICE:2023xif","ALICE:2022ych"],"citeable":true,"imprints":[{"date":"2023-06-05"}],"keywords":[{"value":"Lambda/c+: production","schema":"INSPIRE"},{"value":"yield: ratio","schema":"INSPIRE"},{"value":"parton: distribution function","schema":"INSPIRE"},{"value":"yield: measured","schema":"INSPIRE"},{"value":"charm: hadronization","schema":"INSPIRE"},{"value":"heavy ion: scattering","schema":"INSPIRE"},{"value":"down: production","schema":"INSPIRE"},{"value":"p p: scattering","schema":"INSPIRE"},{"value":"hadron hadron: interaction","schema":"INSPIRE"},{"value":"experimental results","schema":"INSPIRE"},{"value":"5020 GeV-cms/nucleon ","schema":"INSPIRE"}],"refereed":true,"abstracts":[{"value":"The production of prompt baryons has been measured at midrapidity in the transverse momentum interval for the first time, in and –Pb collisions at a center-of-mass energy per nucleon-nucleon collision . The measurement was performed in the decay channel by applying new decay reconstruction techniques using a Kalman-Filter vertexing algorithm and adopting a machine-learning approach for the candidate selection. The -integrated production cross sections in both collision systems were determined and used along with the measured yields in Pb–Pb collisions to compute the -integrated nuclear modification factors and of baryons, which are compared to model calculations that consider nuclear modification of the parton distribution functions. The baryon-to-meson yield ratio is reported for and –Pb collisions. Comparisons with models that include modified hadronization processes are presented, and the implications of the results on the understanding of charm hadronization in hadronic collisions are discussed. 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