Abstract

Recent studies reveal that at high energies, collisions of a small system such as $p+p$ gives signatures similar to that widely observed in heavy ion collisions hinting toward the possibility of forming a medium with collective behavior. With this motivation, we have used the Glauber model, which is traditionally applied to heavy ion collisions, in a small system using the anisotropic and inhomogeneous density profile of a proton and found that the proposed model reproduces the charged particle multiplicity distribution of $p+p$ collisions at LHC energies very well. Collision geometric properties such as the mean impact parameter, the mean number of binary collisions ($⟨{N}_{\mathrm{coll}}⟩$), and the mean number of participants ($⟨{N}_{\mathrm{part}}⟩$) at different multiplicities are determined. Having estimated $⟨{N}_{\mathrm{coll}}⟩$, we have calculated the nuclear modificationlike factor (${R}_{\mathrm{HL}}$) in $p+p$ collisions. We also estimated eccentricity and elliptic flow as a function of charged particle multiplicity using the linear response to the initial geometry.

Highlights

  • Results of relativistic proton proton (p þ p) collisions are used as a reference or base line for interpreting various results of heavy ion collisions at relativistic energies, which are aimed at creation and characterization of phases of strongly interacting matter governed by quantum chromodynamics (QCD)

  • Values of the ratio of a certain observable measured in heavy ion collisions, such as the number of produced strange particles, production of J=ψ, to those measured in the p þ p collision are interpreted as a signature of the partonic medium formation in heavy ion collisions; e.g., the enhancement of the number of strange particles and suppression in the number of J=ψ in collisions of the heavy ion with respect to that of p þ p are taken as signatures of quark-gluon plasma (QGP) formation in relativistic heavy

  • We present the results of Glauber-like model calculations for NcollðbÞ, NpartðbÞ due to the quark and gluon based proton density profile, which is a realistic picture obtained by results of deep inelastic scattering that reveals the structure of the proton [21], and we used it to ocobltlaiisniocnhsaargt epd ffispffi a1⁄4rti7clTeemVu. lCtipalliccuitlyateddistmriubluttiipolniciitny pþp distribution is contrasted with ALICE data, a relation of an impact parameter with multiplicity is calculated, and the multiplicity distribution of eccentricity and flow harmonics is estimated for p þ p collisions

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Summary

INTRODUCTION

Results of relativistic proton proton (p þ p) collisions are used as a reference or base line for interpreting various results of heavy ion collisions at relativistic energies, which are aimed at creation and characterization of phases of strongly interacting matter governed by quantum chromodynamics (QCD). Of any observable expressed by the number of participating nucleons in the collision, NpartðbÞ; (ii) the number of binary nucleon-nucleon collisions, NcollðbÞ used to derive the nuclear modification factor (RAA) from the ratio of AA over pp spectra; (iii) the elliptic and triangular flow parameters (v2) and (v3) normalized by the eccentricity ε2ðbÞ and triangulation ε3ðbÞ of the overlap region; and (iv) the average surface area, AðbÞ; and (v) path length, LðbÞ of the interaction region, knowing the nuclear overlap function TAAðbÞ is important This overlap function depends on a realistic model of the collision geometry [19]. Initial conditions for heavy ion collisions are modeled in two kinds of distinct approaches: (i) one considers nucleonic or partonic collisions for energy deposition in the collision zone, and those are based on Glauber model [21,22,23,24], and (ii) QCD based calculations are employed to estimate initial energy deposition by gluonic fields originated from partonic currents of colliding nuclei [25].

GLAUBER FORMALISM
Calculation of thickness function and overlap function
Calculation of Ncoll and Npart
RESULTS
Charged particle multiplicity estimation
Centrality estimation
The ratio RHL for high to low multiplicity events
Estimation of elliptic flow
SUMMARY AND DISCUSSION

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