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  • B. Alessandro; P. Antonioli; S. Arcelli; X. Bai; N. Bastid; A. Berdnikova; L. Betev; B. Bhattacharjee; L. Bianchi; P. Braun-Munzinger; D. Budnikov; A. Caliva; P. Camerini; M. Carabas; S. Chandra; V. Chibante Barroso; C. H. Christensen; P. Christiansen; Z. Conesa del Valle; P. Crochet; P. Das; B. Diab; D. U. Dixit; A. Dubla; D. Evans; L. Fabbietti; J. Faivre; F. Fan; C. Ferrero; V. J. G. Feuillard; I. Fokin; E. Frajna; M. B. Gay Ducati; E. Glimos; D. J. Q. Goh; N. A. Grunwald; G. G. Guardiano; L. Gyulai; A. Hamdi; B. G. Hanley; P. Hauer; A. Jusko; M. J. Kabus; M. Keil; A. Khatun; S. Kirsch; I. Kisel; J. Klein; M. Kleiner; T. Klemenz; V. Kozhuharov; E. Kryshen; T. M. Lelek; R. C. Lemmon; S. K. Malik; G. Martínez García; M. Masera; C. Mayer; J. E. Mdhluli; M. Meres; S. Monira; I. Morozov; T. Mrnjavac; Y. Pachmayer; S. Perciballi; V. Petrov; S. Piano; P. Pillot; K. K. Pradhan; T. A. Rancien; S. S. Räsänen; A. Rossi; A. Rustamov; Y. Ryabov; J. Ryu; P. Saha; S. K. Saha; B. Sahoo; P. Sarma; R. Schicker; C. Schmidt; K. Schweda; G. Scioli; J. J. Seo; M. Sharma; S. Sharma; R. Singh; T. Sinha; I. Storehaug; L. A. Tarasovicova; A. G. Torres Ramos; W. H. Trzaska; T. S. Tveter; L. Vermunt; M. Verweij; J. Vrláková; B. Windelband; M. Winn; R. Xu; A. K. Yadav

    The journal of high energy physics, 12/2023, Volume: 2023, Issue: 12
    Journal Article

    Abstract Measurements of the production cross sections of prompt D0, D+, D*+, D s + $$ {\textrm{D}}_{\textrm{s}}^{+} $$ , Λ c + $$ {\Lambda}_{\textrm{c}}^{+} $$ , and Ξ c + $$ {\Xi}_{\textrm{c}}^{+} $$ charm hadrons at midrapidity in proton-proton collisions at s $$ \sqrt{s} $$ = 13 TeV with the ALICE detector are presented. The D-meson cross sections as a function of transverse momentum (p T) are provided with improved precision and granularity. The ratios of p T-differential meson production cross sections based on this publication and on measurements at different rapidity and collision energy provide a constraint on gluon parton distribution functions at low values of Bjorken-x (10 −5–10 −4). The measurements of Λ c + $$ {\Lambda}_{\textrm{c}}^{+} $$ ( Ξ c + $$ {\Xi}_{\textrm{c}}^{+} $$ ) baryon production extend the measured p T intervals down to p T = 0(3) GeV/c. These measurements are used to determine the charm-quark fragmentation fractions and the c c ¯ $$ \textrm{c}\overline{\textrm{c}} $$ production cross section at midrapidity (|y| < 0.5) based on the sum of the cross sections of the weakly-decaying ground-state charm hadrons D0, D+, D s + $$ {\textrm{D}}_{\textrm{s}}^{+} $$ , Λ c + $$ {\Lambda}_{\textrm{c}}^{+} $$ , Ξ c 0 $$ {\Xi}_{\textrm{c}}^0 $$ and, for the first time, Ξ c + $$ {\Xi}_{\textrm{c}}^{+} $$ , and of the strongly-decaying J/ψ mesons. The first measurements of Ξ c + $$ {\Xi}_{\textrm{c}}^{+} $$ and Σ c 0 , + + $$ {\Sigma}_{\textrm{c}}^{0,++} $$ fragmentation fractions at midrapidity are also reported. A significantly larger fraction of charm quarks hadronising to baryons is found compared to e+e − and ep collisions. The c c ¯ $$ \textrm{c}\overline{\textrm{c}} $$ production cross section at midrapidity is found to be at the upper bound of state-of-the-art perturbative QCD calculations.