Abstract

In this paper, we investigate the hydrodynamic collectivity in proton-proton collisions at sqrt{s}= 13 TeV, using iEBE-VISHNU with three different initial conditions, namely, HIJING, super-MC and TRENTo. With properly tuned parameters, hydrodynamics gives reasonable descriptions of the measured two-particle correlations, including the integrated and p_mathrm{T}-differential flow. However, the hydrodynamic simulations fail to describe the negative four-particle cumulant c_2^v{4} as measured in experiments. The four-particle cumulant c_2^v{4} is always positive after hydrodynamic evolutions. Further investigations show that the non-linear response between the final v_2 and the initial varepsilon _2 becomes significant in p-p systems. This leads to a large deviation from linear eccentricity scaling and generates additional flow fluctuations, which results in a positive c_2^v{4} even with a negative c_2^varepsilon {4} from the initial state. We also presented the first hydrodynamic calculations of mixed harmonic azimuthal correlations in p-p collisions. Although many qualitative features are reproduced by the hydrodynamic simulations, the measured negative normalized Symmetric-Cumulant nsc_{2,3}{4} cannot be reproduced. Obviously hydrodynamic calculations have a general difficulty to describe the data. It triggers that whether hydrodynamics with a new initial state could solve this puzzle, or hydrodynamics itself is not the appreciated mechanism of the observed collectivity, and the non-hydrodynamic modes become important in p-p collisions at the LHC.

Highlights

  • Ultra-relativistic collisions of heavy ions are intended to create a novel state of matter, the Quark-Gluon Plasma (QGP), and to study its properties

  • Further investigations show that the non-linear response between the final v2 and the initial ε2 becomes significant in p-p systems. This leads to a large deviation from linear eccentricity scaling and generates additional flow fluctuations, which results in a positive c2v{4} even with a negative c2ε{4} from the initial state

  • Extensive measurements of various flow observables performed at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC) together with the successful descriptions from hydrodynamic calculations revealed that the created QGP fireball behaves like a nearly perfect liquid with very small specific shear viscosity [1,2,3,4,5,6,7,8,9,10,11,12,13,14]

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Summary

Introduction

Ultra-relativistic collisions of heavy ions are intended to create a novel state of matter, the Quark-Gluon Plasma (QGP), and to study its properties. Various striking features of collective expansion have been observed in high-multiplicity events of the small collision systems, such as p–Au, d–Au, 3He–Au at RHIC [15,16] and p–p and p–Pb at the LHC [17,18,19] These features include the long-range “double ridge” structures in two-particle azimuthal correlations with a large pseudo-rapidity gap even up to 8 units [20,21,22,23,24,25,26,27,28,29,30,31,32], the changing signs of the 4-particle cumulants [15,27,28,29,30,31,32,33,34] and v2 mass ordering of identified hadrons [30,35,36,37], etc.

The model and set-ups
TRENTo initial condition
Results and discussion
Summary
Full Text
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