Evolution of fluctuations in the initial state of heavy-ion collisions from RHIC to LHC

6533b7d0fe1ef96bd125a548

RESEARCH PRODUCT

Evolution of fluctuations in the initial state of heavy-ion collisions from RHIC to LHC

Francçois Gelis Cyrille Marquet Jean-yves Ollitrault Giuliano Giacalone Pablo Guerrero-rodríguez Matthew Luzum

subject

heavy ion: scattering Scale (ratio)Field (physics)Nuclear Theory [PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciences [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy 01 natural sciences Color-glass condensate High Energy Physics - Experiment Nuclear physics Nuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences Effective field theory [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)010306 general physics initial state Nuclear Experiment Nuclear Experiment Brookhaven RHIC Coll Physics Large Hadron Collider 010308 nuclear & particles physics fluctuation elliptic flow particle: multiplicity Elliptic flow Observable High Energy Physics - Phenomenology CERN LHC Coll [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]color glass condensate Particle scale: saturation

description

Fluctuations in the initial state of heavy-ion collisions are larger at RHIC energy than at LHC energy. This fact can be inferred from recent measurements of the fluctuations of the particle multiplicities and of elliptic flow performed at the two different energies. We show that an analytical description of the initial energy-density field and its fluctuations motivated by the color glass condensate (CGC) effective theory predicts and quantitatively captures the measured energy evolution of these observables. The crucial feature is that fluctuations in the CGC scale like the inverse of the saturation scale of the nuclei.

year	journal	country	edition	language
2019-12-04

https://dx.doi.org/10.48550/arxiv.1911.04720

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