scholarly journals Estimation of stopped protons at energies relevant for a beam energy scan at the BNL Relativistic Heavy Ion Collider

2017 ◽  
Vol 95 (4) ◽  
Author(s):  
Dhananjaya Thakur ◽  
Sunil Jakhar ◽  
Prakhar Garg ◽  
Raghunath Sahoo
Keyword(s):  
Beam Energy ◽  
Heavy Ion ◽  
Relativistic Heavy Ion Collider ◽  
Beam Energy Scan

scholarly journals Quark Number Susceptibilities and Equation of State in QCD at Finite μB

Proceedings ◽  
2019 ◽  
Vol 13 (1) ◽  
pp. 5
Author(s):  
Saumen Datta ◽  
Rajiv Gavai ◽  
Sourendu Gupta
Keyword(s):  
Equation Of State ◽  
Taylor Series ◽  
Chemical Potential ◽  
Baryon Number ◽  
Heavy Ion ◽  
Relativistic Heavy Ion Collider ◽  
Quark Number ◽  
Monte Carlo Studies ◽  
Essential Input ◽  
Beam Energy Scan

One of the main goals of the cold baryonic matter (CBM) experiment at FAIR is to explore the phases of strongly interacting matter at finite temperature and baryon chemical potential μ B . The equation of state of quantum chromodynamics (QCD) at μ B > 0 is an essential input for the CBM experiment, as well as for the beam energy scan in the Relativistic Heavy Ion Collider(RHIC) experiment. Unfortunately, it is highly nontrivial to calculate the equation of state directly from QCD: numerical Monte Carlo studies on lattice are not useful at finite μ B . Using the method of Taylor expansion in chemical potential, we estimate the equation of state, namely the baryon number density and its contribution to the pressure, for two-flavor QCD at moderate μ B . We also study the quark number susceptibilities. We examine the technicalities associated with summing the Taylor series, and explore a Pade resummation. An examination of the Taylor series can be used to get an estimate of the location of the critical point in μ B , T plane.

Strange particle effective temperatures in relativistic nuclear collisions

2020 ◽  
Vol 29 (02) ◽  
pp. 2050009
Author(s):  
Oana Ristea ◽  
Catalin Ristea ◽  
Alexandru Jipa
Keyword(s):  
Energy Dependence ◽  
Sudden Change ◽  
Heavy Ion ◽  
Strange Particle ◽  
Relativistic Heavy Ion Collider ◽  
Nuclear Collisions ◽  
Effective Temperatures ◽  
Relativistic Nuclear Collisions ◽  
Onset Of Deconfinement ◽  
Beam Energy Scan

The energy dependence of the effective temperatures of charged kaons, [Formula: see text] and [Formula: see text] produced in Au[Formula: see text]Au collisions at the Relativistic Heavy Ion Collider (RHIC) Beam Energy Scan (BES) energies are presented. At energies around [Formula: see text][Formula: see text]GeV, there is a sudden change in the energy dependence of [Formula: see text] and [Formula: see text] effective temperatures, while at higher energies a slower, continuous rise up to [Formula: see text][Formula: see text]TeV is observed. This behavior is similar with previous SPS results and could indicate the onset of deconfinement in this energy range. The [Formula: see text] effective temperatures increase with energy and no plateau-like behavior is evidenced by the data.

scholarly journals Centrality Dependence of Chemical Freeze-Out Parameters and Strangeness Equilibration in RHIC and LHC Energies

2021 ◽  
Vol 2021 ◽  
pp. 1-15
Author(s):  
Deeptak Biswas
Keyword(s):  
Hadron Collider ◽  
Heavy Ion ◽  
Strange Particle ◽  
Relativistic Heavy Ion Collider ◽  
Yield Data ◽  
Central Collisions ◽  
Chemical Potentials ◽  
Beam Energy Scan ◽  
Chemical Freeze ◽  
Freeze Out

We have estimated centrality variation of chemical freeze-out parameters from yield data at midrapidity of π ± , K ± and p , p ¯ for collision energies of RHIC (Relativistic Heavy Ion Collider), Beam Energy Scan (RHIC-BES) program, and LHC (Large Hadron Collider). We have considered a simple hadron resonance gas model and employed a formalism involving conserved charges ( B , Q , S ) of QCD for parameterization. Along with temperature and three chemical potentials ( T , μ B , μ Q , μ S ), a strangeness undersaturation factor ( γ S ) has been used to incorporate the partial equilibration in the strange sector. Our obtained freeze-out temperature does not vary much with centrality, whereas chemical potentials and γ S seem to have a significant dependence. The strange hadrons are found to deviate from a complete chemical equilibrium at freeze-out at the peripheral collisions. This deviation appears to be more prominent as the collision energy decreases at lower RHIC-BES energies. We have also shown that this departure from equilibrium reduces towards central collisions, and strange particle equilibration may happen after a threshold number of participants in A - A collision.

scholarly journals Review of Critical Point Searches and Beam-Energy Studies

Proceedings ◽  
2019 ◽  
Vol 10 (1) ◽  
pp. 8 ◽  
Author(s):  
Fabian Rennecke
Keyword(s):  
Phase Diagram ◽  
Critical Point ◽  
Beam Energy ◽  
Particle Number ◽  
Phase Diagram Of Qcd ◽  
Theoretical Perspective ◽  
Heavy Ion ◽  
Ion Collisions ◽  
Introductory Overview ◽  
Beam Energy Scan

I give an introductory overview of the search for the critical point in the phase diagram of QCD in the context of heavy-ion collisions from a theoretical perspective. The focus is on static and dynamic critical physics and the corresponding properties of particle number fluctuations as relevant examples of promising observables for signatures of a critical point in beam-energy scan experiments.

scholarly journals A Study of the Properties of the QCD Phase Diagram in High-Energy Nuclear Collisions

Particles ◽  
2020 ◽  
Vol 3 (2) ◽  
pp. 278-307 ◽  
Author(s):  
Xiaofeng Luo ◽  
Shusu Shi ◽  
Nu Xu ◽  
Yifei Zhang
Keyword(s):  
Heavy Ion ◽  
High Energy ◽  
Baryon Density ◽  
Heavy Flavor ◽  
Relativistic Heavy Ion Collider ◽  
Density Region ◽  
Nuclear Collisions ◽  
Qcd Phase Diagram ◽  
Beam Energy Scan ◽  
Ion Collision

With the aim of understanding the phase structure of nuclear matter created in high-energy nuclear collisions at finite baryon density, a beam energy scan program has been carried out at Relativistic Heavy Ion Collider (RHIC). In this mini-review, most recent experimental results on collectivity, criticality and heavy flavor productions will be discussed. The goal here is to establish the connection between current available data and future heavy-ion collision experiments in a high baryon density region.

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