Search results for "NEAR-SIDE"

showing 3 items of 3 documents

Hot spots and gluon field fluctuations as causes of eccentricity in small systems

2021

We calculate eccentricities in high energy proton-nucleus collisions, by calculating correlation functions of the energy density field of the Glasma immediately after the collision event at proper time tau = 0. We separately consider the effects of color charge and geometrical hot spot fluctuations, analytically performing the averages over both in a dilute-dense limit. We show that geometric fluctuations of hot spots inside the proton are the dominant source of eccentricity whereas color charge fluctuations only give a negligible correction. The size and number of hot spots are the most important parameters characterizing the eccentricities.

Nuclear TheoryField (physics)ProtonAZIMUTHAL ANISOTROPIESFLOWmedia_common.quotation_subjectFOS: Physical sciencesHot spot (veterinary medicine)hiukkasfysiikka114 Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesProper timeEccentricity (behavior)LONG-RANGEHARMONICSNuclear Experiment010306 general physicsPLUS PB COLLISIONSGluon fieldmedia_commonPROTON-LEAD COLLISIONSPhysics010308 nuclear & particles physicskvarkki-gluoniplasmaANGULAR-CORRELATIONSComputational physicsHigh Energy Physics - PhenomenologyNEAR-SIDEAstrophysics::Earth and Planetary AstrophysicsHIGH TRANSVERSE-MOMENTUMPPBEvent (particle physics)Color chargePhysical Review D
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Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at √sNN = 2.76 TeV

2017

In two-particle angular correlation measurements, jets give rise to a near-side peak, formed by particles associated to a higher-pT trigger particle. Measurements of these correlations as a function of pseudorapidity (η) and azimuthal (ϕ) differences are used to extract the centrality and pT dependence of the shape of the near-side peak in the pT range 1 < pT < 8 GeV/c in Pb-Pb and pp collisions at √sNN = 2.76 TeV. A combined fit of the near-side peak and long-range correlations is applied to the data and the peak shape is quantified by the variance of the distributions. While the width of the peak in the ϕ direction is almost independent of centrality, a significant broadening in the η dir…

Nuclear and High Energy Physicsnear-side jet peakPb-Pb collisionshiukkasfysiikkaNuclear Experiment
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"Table 6" of "Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV"

2021

No table description available.

P P --&gt; d X13000.0Near-side yield
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