Abstract
The measurement of prompt D-meson production as a function of multiplicity in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV with the ALICE detector at the LHC is reported. D$^0$, D$^+$ and D$^{*+}$ mesons are reconstructed via their hadronic decay channels in the centre-of-mass rapidity range $-0.96< y_{\mathrm{cms}}<0.04$ and transverse momentum interval $1<p_{\rm T}<24$ GeV/$c$. The multiplicity dependence of D-meson production is examined by either comparing yields in p-Pb collisions in different event classes, selected based on the multiplicity of produced particles or zero-degree energy, with those in pp collisions, scaled by the number of binary nucleon-nucleon collisions (nuclear modification factor); as well as by evaluating the per-event yields in p-Pb collisions in different multiplicity intervals normalised to the multiplicity-integrated ones (relative yields). The nuclear modification factors for D$^0$, D$^+$ and D$^{*+}$ are consistent with one another. The D-meson nuclear modification factors as a function of the zero-degree energy are consistent with unity within uncertainties in the measured $p_{\rm T}$ regions and event classes. The relative D-meson yields, calculated in various $p_{\rm T}$ intervals, increase as a function of the charged-particle multiplicity. The results are compared with the equivalent pp measurements at $\sqrt{s}=7$ TeV as well as with EPOS~3 calculations.
Highlights
Multiplicity in p–Pb collisions at sNN = 5.02 TeV with the ALICE detector at the LHC is reported
Inclusive charm meson production measurements at the LHC [19,20,21] are reproduced within uncertainties by the predictions of GM-VFNS, Fixed-Order plus Next-to-Leading Logarithms (FONLL) and those performed in the framework of kT factorisation in the Leading Order (LO) approximation [22]
It is worth noting that the smaller number of reconstructed D mesons in the lowest and highest pT intervals1 limited the number of multiplicity intervals of the measurement for those pT intervals
Summary
The ALICE apparatus is described in detail in [61] and its performance in [62] It is composed of a series of detectors in the central barrel for tracking and particle identification; the Muon Spectrometer in the forward direction for muon tracking and identification; and a further set of detectors at forward rapidity for triggering and event characterisation. The Inner Tracking System (ITS), the Time Projection Chamber (TPC) and the Time Of Flight detector (TOF) allow the reconstruction and identification of charged particles in the central pseudorapidity region. The TPC is a large cylindrical drift detector, extending from 85 cm to 247 cm in the radial direction and covering the range −250 < z < +250 cm along the beam axis [64] It provides charged-particle trajectory reconstruction with up to 159 space points per track in the pseudorapidity range |η| < 0.9 and in the full azimuth.
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