1,528 research outputs found
Transverse energy and charged particle production in heavy-ion collisions: From RHIC to LHC
We study the charged particle and transverse energy production mechanism from
AGS, SPS, RHIC to LHC energies in the framework of nucleon and quark
participants. At RHIC and LHC energies, the number of nucleons-normalized
charged particle and transverse energy density in pseudorapidity, which shows a
monotonic rise with centrality, turns out to be an almost centrality
independent scaling behaviour when normalized to the number of participant
quarks. A universal function which is a combination of logarithmic and
power-law, describes well the charged particle and transverse energy production
both at nucleon and quark participant level for the whole range of collision
energies. Energy dependent production mechanisms are discussed both for
nucleonic and partonic level. Predictions are made for the pseudorapidity
densities of transverse energy, charged particle multiplicity and their ratio
(the barometric observable, ) at mid-rapidity for Pb+Pb collisions
at TeV. A comparison with models based on gluon
saturation and statistical hadron gas is made for the energy dependence of
.Comment: 19 pages, 7 figure
A new description of transverse momentum spectra of identified particles produced in proton-proton collisions at high energies
The transverse momentum spectra of identified particles produced in high
energy proton-proton () collisions are empirically described by a new
method with the framework of participant quark model or the multisource model
at the quark level, in which the source itself is exactly the participant
quark. Each participant (constituent) quark contributes to the transverse
momentum spectrum, which is described by the TP-like function, a revised
Tsallis--Pareto-type function. The transverse momentum spectrum of the hadron
is the convolution of two or more TP-like functions. For a lepton, the
transverse momentum spectrum is the convolution of two TP-like functions due to
two participant quarks, e.g. projectile and target quarks, taking part in the
collisions. A discussed theoretical approach seems to describe the
collisions data at center-of-mass energy GeV, 2.76 TeV, and 13
TeV very well.Comment: 19 pages, 7 figures. Advances in High Energy Physics, accepte
Time Evolution of Temperature Fluctuation in a Non-Equilibrated System
The evolution equation for inhomogeneous and anisotropic temperature
fluctuation inside a medium is derived within the ambit of Boltzmann Transport
Equation (BTE) for a hot gas of massless particles. Also, specializing to a
situation created after heavy-ion collision (HIC), we analyze the Fourier space
variation of temperature fluctuation of the medium using its temperature
profile. The effect of viscosity on the variation of fluctuations in the latter
case is investigated and possible implications for early universe cosmology,
and its connection with HICs are also explored.Comment: 5 pages, 5 figures, Minor changes in the tex
Constituent Quark Scaling of Strangeness Enhancement in Heavy-Ion Collisions
In the frame work of a nuclear overlap model, we estimate the number of
nucleon and quark participants in proton-proton, proton-nucleus and
nucleus-nucleus collisions. We observe the number of nucleon
()-normalized enhancement of multi-strange particles which show a
monotonic increase with centrality, turns out to be a centrality independent
scaling behavior when normalized to number of constituent quarks participating
in the collision (). In addition, we observe that the
-normalized enhancement, when further normalized to the strangeness
content, shows a strangeness independent scaling behavior. This holds good at
top RHIC energy. However, the corresponding SPS data show a weak
-scaling with strangeness scaling being violated at top SPS energy.
This scaling at RHIC indicates that the partonic degrees of freedom playing an
important role in the production of multi-strange particles. Top SPS energy, in
view of the above observations, shows a co-existence of hadronic and partonic
phases. We give a comparison of data with HIJING, AMPT and UrQMD models to
understand the particle production dynamics at different energies.Comment: 9 pages, 17 figure
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