Multiparton interactions (MPI) in pp collisions have attracted the attention of the heavy-ion community since they can help to elucidate the origin of collectivelike effects discovered in small collision systems at the LHC. In this work, we report that in PYTHIA8.244, the charged-particle production in events with a large number of MPI (N mpi) normalized to that obtained in minimum-bias pp collisions shows interesting features. After the normalization to the corresponding hN mpi i, the ratios as a function of p T exhibit a bump at p T ≈ 3 GeV=c; and for higher p T (> 8 GeV=c), the ratios are independent of N mpi. While the size of the bump increases with increasing N mpi , the behavior at high p T is expected from the "binary scaling" (partonparton interactions), which holds given the absence of any parton-energy loss mechanism in PYTHIA. The bump at intermediate p T is reminiscent of the Cronin effect observed for the nuclear modification factor in p-Pb collisions. In order to unveil these effects in data, we propose a strategy to construct an event classifier sensitive to MPI using machine learning-based regression. The study is conducted using TMVA, and the regression is performed with boosted decision trees (BDT). Event properties like forward charged-particle multiplicity, transverse spherocity and the average transverse momentum (hp T i) are used for training. The kinematic cuts are defined in accordance with the ALICE detector capabilities. For the validation of the method and to find possible model dependence, we also compare the results from PYTHIA8.244 with HERWIG7.1. In addition, we also report that if we apply the trained BDT on existing (INEL > 0) pp data, i.e., events with at least one primary charged-particle within jηj < 1, the average number of MPI in pp collisions at ffiffi ffi s p ¼ 5.02 and 13 TeV are 3.76 AE 1.01 and 4.65 AE 1.01, respectively.

No abstract

No abstract

No abstract

The azimuthal ($$\Delta \varphi $$ Δ φ ) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p–Pb collisions at $$\sqrt{s_{\mathrm{{NN}}}} = 5.02$$ s NN = 5.02 TeV. Results are reported for electrons with transverse momentum $$4<p_{\textrm{T}}<16$$ 4 < p T < 16 $$\textrm{GeV}/c$$ GeV / c  and pseudorapidity $$|\eta |<0.6$$ | η | < 0.6 . The associated charged particles are selected with transverse momentum $$1<p_{\textrm{T}}<7$$ 1 < p T < 7 $$\textrm{GeV}/c$$ GeV / c , and relative pseudorapidity separation with the leading electron $$|\Delta \eta | < 1$$ | Δ η | < 1 . The correlation measurements are performed to study and characterize the fragmentation and hadronization of heavy quarks. The correlation structures are fitted with a constant and two von Mises functions to obtain the baseline and the near- and away-side peaks, respectively. The results from p–Pb collisions are compared with those from pp collisions to study the effects of cold nuclear matter. In the measured trigger electron and associated particle kinematic regions, the two collision systems give consistent results. The $$\Delta \varphi $$ Δ φ distribution and the peak observables in pp and p–Pb collisions are compared with calculations from various Monte Carlo event generators.