33 research outputs found

    Investigating the mechanism of hadron production by measuring angular correlations of mesons with hidden strangeness in the ALICE experiment

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    Hadronization is a process described by quantum chromodynamics in which hadrons are formed from quarks and gluons. Given the non-perturbative nature of this phenomenon, it is not yet fully understood. To study this effect, we can only use phenomenological models. Such phenomenological models are characterized by the fact that the parameters used to describe them are obtained from experimental data. Initial attempts to model this process in particle collisions can be found as early as 1977, but the study of this phenomenon continues to this day. The angular correlations are a powerful tool for studying the physics of heavy ions as well as lighter systems, such as protons. The correlations of the functions Δη\Delta \eta and Δφ\Delta \varphi (the difference in pseudorapidity and azimuthal angle, respectively) are sensitive to contributions from various physical effects. The purpose of the analyses is to derive the influences of specific physical effects on the final angular correlation function. Using simulations, we have knowledge of what shapes in space (Δη\Delta \eta, Δφ\Delta \varphi ) we can expect from particular physical effects. In terms of its particle identification capabilities, the ALICE experiment is an ideal tool for performing correlation analyses for different particles. Following the extensive changes made to the ALICE experiment's detector system, it was necessary to introduce new data analysis software -- ALICE O2O^2. Along with the change in the analysis software, the format of the data and its processing have also changed. Thanks to the use of Appache Arrow flat arrays, declarative programming methods and the C++ 17 language, it allows for a reduction in the resources used and a speeding up of the analysis time. The existing research conducted in the field of angular correlations indicates that the process of hadronization of baryons may proceed differently from the process of meson production. This thesis intends to answer the question of whether mass affects the hadronization process by analyzing the angular correlations of mesons with similar mass to the lightest baryon, which is a proton

    Measurement of the impact-parameter dependent azimuthal anisotropy in coherent ρ0 photoproduction in Pb–Pb collisions at √sNN = 5.02 TeV

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    The first measurement of the impact-parameter dependent angular anisotropy in the decay of coherently photoproduced ρ0 mesons is presented. The ρ0 mesons are reconstructed through their decay into a pion pair. The measured anisotropy corresponds to the amplitude of the cos(2ϕ) modulation, where ϕ is the angle between the two vectors formed by the sum and the difference of the transverse momenta of the pions, respectively. The measurement was performed by the ALICE Collaboration at the LHC using data from ultraperipheral Pb−Pb collisions at a center-of-mass energy of sNN−−−√ = 5.02 TeV per nucleon pair. Different impact-parameter regions are selected by classifying the events in nuclear-breakup classes. The amplitude of the cos(2ϕ) modulation is found to increase by about one order of magnitude from large to small impact parameters. Theoretical calculations, which describe the measurement, explain the cos(2ϕ) anisotropy as the result of a quantum interference effect at the femtometer scale that arises from the ambiguity as to which of the nuclei is the source of the photon in the interaction

    Exclusive four pion photoproduction in ultraperipheral Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV

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    International audienceThe intense photon fluxes from relativistic nuclei provide an opportunity to study photonuclear interactions in ultraperipheral collisions. The measurement of coherently photoproduced π+ππ+π\pi^+\pi^-\pi^+\pi^- final states in ultraperipheral Pb-Pb collisions at sNN=5.02\sqrt{s_{\mathrm{NN}}}=5.02 TeV is presented for the first time. The cross section, dσ\sigma/dyy, times the branching ratio (ρπ+π+ππ\rho\rightarrow \pi^+ \pi^+ \pi^- \pi^-) is found to be 47.8±2.3 (stat.)±7.7 (syst.)47.8\pm2.3~\rm{(stat.)}\pm7.7~\rm{(syst.)} mb in the rapidity interval y<0.5|y| < 0.5. The invariant mass distribution is not well described with a single Breit-Wigner resonance. The production of two interfering resonances, ρ(1450)\rho(1450) and ρ(1700)\rho(1700), provides a good description of the data. The values of the masses (mm) and widths (Γ\Gamma) of the resonances extracted from the fit are m1=1385±14 (stat.)±3 (syst.)m_{1}=1385\pm14~\rm{(stat.)}\pm3~\rm{(syst.)} MeV/c2c^2, Γ1=431±36 (stat.)±82 (syst.)\Gamma_{1}=431\pm36~\rm{(stat.)}\pm82~\rm{(syst.)} MeV/c2c^2, m2=1663±13 (stat.)±22 (syst.)m_{2}=1663\pm13~\rm{(stat.)}\pm22~\rm{(syst.)} MeV/c2c^2 and Γ2=357±31 (stat.)±49 (syst.)\Gamma_{2}=357 \pm31~\rm{(stat.)}\pm49~\rm{(syst.)} MeV/c2c^2, respectively. The measured cross sections times the branching ratios are compared to recent theoretical predictions

    Measurement of the production cross section of prompt Ξ0c baryons in p–Pb collisions at √sNN = 5.02 TeV

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    The transverse momentum (pT) differential production cross section of the promptly-produced charm-strange baryon Ξ0c (and its charge conjugate Ξ0c¯¯¯¯¯¯) is measured at midrapidity via its hadronic decay into π+Ξ− in p−Pb collisions at a centre-of-mass energy per nucleon−nucleon collision sNN−−−√ = 5.02 TeV with the ALICE detector at the LHC. The Ξ0c nuclear modification factor (RpPb), calculated from the cross sections in pp and p−Pb collisions, is presented and compared with the RpPb of Λ+c baryons. The ratios between the pT-differential production cross section of Ξ0c baryons and those of D0 mesons and Λ+c baryons are also reported and compared with results at forward and backward rapidity from the LHCb Collaboration. The measurements of the production cross section of prompt Ξ0c baryons are compared with a model based on perturbative QCD calculations of charm-quark production cross sections, which includes only cold nuclear matter effects in p−Pb collisions, and underestimates the measurement by a factor of about 50. This discrepancy is reduced when the data is compared with a model in which hadronisation is implemented via quark coalescence. The pT-integrated cross section of prompt Ξ0c-baryon production at midrapidity extrapolated down to pT = 0 is also reported. These measurements offer insights and constraints for theoretical calculations of the hadronisation process. Additionally, they provide inputs for the calculation of the charm production cross section in p−Pb collisions at midrapidity

    Measurement of Ω0c baryon production and branching-fraction ratio BR(Ω0c → Ω−e+νe)/BR(Ω0c → Ω−π+) in pp collisions at √s = 13 TeV

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    The inclusive production of the charm-strange baryon Ω0c is measured for the first time via its semileptonic decay into Ω−e+νe at midrapidity (|y| < 0.8) in proton–proton (pp) collisions at the centre-of-mass energy √s = 13 TeV with the ALICE detector at the LHC. The transverse momentum (pT) differential cross section multiplied by the branching ratio is presented in the interval 2 < pT < 12 GeV/c. The branching-fraction ratio BR(Ω0c → Ω−e+νe)/BR(Ω0c → Ω−π+) is measured to be 1.12 ± 0.22 (stat.) ± 0.27 (syst.). Comparisons with other experimental measurements, as well as with theoretical calculations, are presented

    K∗(892)± resonance production in Pb−Pb collisions at √sNN = 5.02 TeV

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    The production of K∗(892)± meson resonance is measured at midrapidity (|y|8 GeV/c, consistent with measurements for other light-flavored hadrons. The smallest values are observed in most central collisions, indicating larger energy loss of partons traversing the dense medium

    Investigating Λ\Lambda baryon production in p-Pb collisions in jets and underlying event using angular correlations

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    This paper presents the first measurements of hadron(h)Λ-\Lambda azimuthal angular correlations in p-Pb collisions at sNN\sqrt{s_{\rm NN}} = 5.02 TeV using the ALICE detector at the LHC. These correlations are used to separate the production of associated Λ\Lambda baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated Λ\Lambda yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle pTp_{\rm T} and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the ϕ(1020)\phi(1020) meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of Λ\Lambda relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.First measurements of hadron(h)Λ-\Lambda azimuthal angular correlations in p-Pb collisions at sNN\sqrt{s_{\rm NN}} = 5.02 TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated Λ\Lambda baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated Λ\Lambda yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle pTp_{\rm T} and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the ϕ(1020)\phi(1020) meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of Λ\Lambda relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event

    Measurement of Ωc0\Omega^0_{\rm c} baryon production and branching-fraction ratio BR(Ωc0Ωe+νe)/BR(Ωc0Ωπ+){\rm BR(\Omega^0_c \rightarrow \Omega^- e^+\nu_e)} / {\rm BR(\Omega^0_c \rightarrow \Omega^- \pi^+)} in pp collisions at s\sqrt{s} = 13 TeV

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    International audienceThe inclusive production of the charm-strange baryon Ωc0\Omega^{0}_{\rm c} is measured for the first time via its semileptonic decay into Ωe+νe\Omega^{-}\rm e^{+}\nu_{e} at midrapidity (y<0.8|y|<0.8) in proton-proton (pp) collisions at the centre-of-mass energy s=13\sqrt{s}=13 TeV with the ALICE detector at the LHC. The transverse momentum (pTp_{\rm T}) differential cross section multiplied by the branching ratio is presented in the interval 2<pT<12 GeV/c2<p_{\rm T}<12~{\rm GeV}/c. The branching-fraction ratio BR(Ωc0Ωe+νe)/BR(Ωc0Ωπ+){\rm BR}(\Omega^0_{\rm c} \rightarrow \Omega^{-}{\rm e}^{+}\nu_{\rm e})/ {\rm BR}(\Omega^0_{\rm c} \rightarrow \Omega^{-}{\pi}^{+}) is measured to be 1.12 ±\pm 0.22 (stat.) ±\pm 0.27 (syst.). Comparisons with other experimental measurements, as well as with theoretical calculations, are presented

    Systematic study of flow vector decorrelation in sNN=5.02\mathbf{\sqrt{\textit{s}_{_{\bf NN}}}=5.02} TeV Pb-Pb collisions

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    International audienceMeasurements of the pTp_{\rm T}-dependent flow vector fluctuations in Pb-Pb collisions at sNN=5.02 TeV\sqrt{s_{_{\rm NN}}} = 5.02~\mathrm{TeV} using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach [1] is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the pTp_{\rm T}-dependent flow vector fluctuations at sNN=5.02 TeV\sqrt{s_{_{\rm NN}}} = 5.02~\mathrm{TeV} with two-particle correlations. Significant pTp_{\rm T}-dependent fluctuations of the V2\vec{V}_{2} flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to \sim15% being present in the 5% most central collisions. In parallel, no evidence of significant pTp_{\rm T}-dependent fluctuations of V3\vec{V}_{3} or V4\vec{V}_{4} is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than 5σ5\sigma significance in central collisions. These observations in Pb-Pb collisions indicate where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high pTp_{\rm T}, which might be biased by pTp_{\rm T}-dependent flow angle fluctuations of at least 23% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system

    Measurement of Ωc0\Omega^0_{\rm c} baryon production and branching-fraction ratio BR(Ωc0Ωe+νe)/BR(Ωc0Ωπ+){\rm BR(\Omega^0_c \rightarrow \Omega^- e^+\nu_e)} / {\rm BR(\Omega^0_c \rightarrow \Omega^- \pi^+)} in pp collisions at s\sqrt{s} = 13 TeV

    No full text
    International audienceThe inclusive production of the charm-strange baryon Ωc0\Omega^{0}_{\rm c} is measured for the first time via its semileptonic decay into Ωe+νe\Omega^{-}\rm e^{+}\nu_{e} at midrapidity (y<0.8|y|<0.8) in proton-proton (pp) collisions at the centre-of-mass energy s=13\sqrt{s}=13 TeV with the ALICE detector at the LHC. The transverse momentum (pTp_{\rm T}) differential cross section multiplied by the branching ratio is presented in the interval 2<pT<12 GeV/c2<p_{\rm T}<12~{\rm GeV}/c. The branching-fraction ratio BR(Ωc0Ωe+νe)/BR(Ωc0Ωπ+){\rm BR}(\Omega^0_{\rm c} \rightarrow \Omega^{-}{\rm e}^{+}\nu_{\rm e})/ {\rm BR}(\Omega^0_{\rm c} \rightarrow \Omega^{-}{\pi}^{+}) is measured to be 1.12 ±\pm 0.22 (stat.) ±\pm 0.27 (syst.). Comparisons with other experimental measurements, as well as with theoretical calculations, are presented
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