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CERN Accelerating science

 
Upper: distributions of \dphitz in \pp collisions compared to \PbPb collisions (left to right) in the 70--90 (left), 50--70, 30--50, and 0--30\% (right) centrality intervals. Lower: difference between the \PbPb and \pp distributions. The vertical bars and shaded boxes represent the statistical and systematic uncertainties, respectively. Several model calculations are added for comparison: Hybrid~\cite{Casalderrey-Solana:2016jvj} and CoLBT~\cite{Chen:2020tbl,Yang:2021qtl}.
Upper: distributions of \xizt in \pp collisions compared to \PbPb collisions (left to right) in the 70--90 (left), 50--70, 30--50, and 0--30\% (right) centrality intervals. Lower: ratios of the \PbPb to \pp distributions. The vertical bars and shaded boxes represent the statistical and systematic uncertainties, respectively. Several model calculations are added for comparison: Hybrid~\cite{Casalderrey-Solana:2016jvj}, CoLBT~\cite{Chen:2020tbl,Yang:2021qtl}, and \scetg~\cite{Li:2019dre}.
Upper: Distributions of \dNptt in \pp collisions compared to \PbPb collisions (left to right) in the 70--90 (left), 50--70, 30--50, and 0--30\% (right) centrality intervals. Lower: ratios of the \PbPb to \pp distributions. The vertical bars and shaded boxes represent the statistical and systematic uncertainties, respectively. Several model calculations are added for comparison: Hybrid~\cite{Casalderrey-Solana:2016jvj}, CoLBT~\cite{Chen:2020tbl,Yang:2021qtl}, and \scetg~\cite{Li:2019dre}.