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Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach

We have estimated the dimensionless parameters such as Reynolds number (Re), Knudsen number (Kn) and Mach number (Ma) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size depen...

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Autores principales: Scaria, Ronald, Sahu, Dushmanta, Singh, Captain R., Sahoo, Raghunath, Alam, Jan-e
Lenguaje:eng
Publicado: 2022
Materias:
Acceso en línea:https://dx.doi.org/10.1140/epja/s10050-023-01052-1
http://cds.cern.ch/record/2800102
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author Scaria, Ronald
Sahu, Dushmanta
Singh, Captain R.
Sahoo, Raghunath
Alam, Jan-e
author_facet Scaria, Ronald
Sahu, Dushmanta
Singh, Captain R.
Sahoo, Raghunath
Alam, Jan-e
author_sort Scaria, Ronald
collection CERN
description We have estimated the dimensionless parameters such as Reynolds number (Re), Knudsen number (Kn) and Mach number (Ma) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size dependence of these parameters indicate that the system formed in proton+proton collisions may achieve thermal equilibrium making it unsuitable as a benchmark to analyze the properties of the system produced in heavy ion collisions at similar energies. While the magnitude of Kn can be used to study the degree of thermalization and applicability of inviscid hydrodynamics, the variations of Re and Ma with temperature (T) and baryonic chemical potential ($\mu _B$) assist to understand the change in the nature of the flow in the system. Indeed the nature of flow changes from laminar to turbulent as Re increases and the system is characterized as incompressible for low $Ma (<<1)$ and compressible for larger Ma. Ma can also be used to understand whether the flow is subsonic or supersonic.
id cern-2800102
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2022
record_format invenio
spelling cern-28001022023-06-29T03:46:51Zdoi:10.1140/epja/s10050-023-01052-1doi:10.1140/epja/s10050-023-01052-1http://cds.cern.ch/record/2800102engScaria, RonaldSahu, DushmantaSingh, Captain R.Sahoo, RaghunathAlam, Jan-eFluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approachnucl-thNuclear Physics - Theorynucl-exNuclear Physics - Experimenthep-exParticle Physics - Experimenthep-phParticle Physics - PhenomenologyWe have estimated the dimensionless parameters such as Reynolds number (Re), Knudsen number (Kn) and Mach number (Ma) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size dependence of these parameters indicate that the system formed in proton+proton collisions may achieve thermal equilibrium making it unsuitable as a benchmark to analyze the properties of the system produced in heavy ion collisions at similar energies. While the magnitude of Kn can be used to study the degree of thermalization and applicability of inviscid hydrodynamics, the variations of Re and Ma with temperature (T) and baryonic chemical potential ($\mu _B$) assist to understand the change in the nature of the flow in the system. Indeed the nature of flow changes from laminar to turbulent as Re increases and the system is characterized as incompressible for low $Ma (<<1)$ and compressible for larger Ma. Ma can also be used to understand whether the flow is subsonic or supersonic.We have estimated the dimensionless parameters such as Reynolds number ($Re$), Knudsen number ($Kn$) and Mach number ($Ma$) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size dependence of these parameters indicate that the system formed in proton+proton collisions may achieve thermal equilibrium making it unsuitable as a benchmark to analyze the properties of the system produced in heavy ion collisions at similar energies. While the magnitude of $Kn$ can be used to study the degree of thermalization and applicability of inviscid hydrodynamics, the variations of $Re$ and $Ma$ with temperature ($T$) and baryonic chemical potential ($\mu_B$) assist to understand the change in the nature of the flow in the system. Indeed the nature of flow changes from laminar to turbulent as $Re$ increases and the system is characterized as incompressible for low $Ma (<<1)$ and compressible for larger $Ma$. $Ma$ can also be used to understand whether the flow is subsonic or supersonic.arXiv:2201.08096oai:cds.cern.ch:28001022022-01-20
spellingShingle nucl-th
Nuclear Physics - Theory
nucl-ex
Nuclear Physics - Experiment
hep-ex
Particle Physics - Experiment
hep-ph
Particle Physics - Phenomenology
Scaria, Ronald
Sahu, Dushmanta
Singh, Captain R.
Sahoo, Raghunath
Alam, Jan-e
Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach
title Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach
title_full Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach
title_fullStr Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach
title_full_unstemmed Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach
title_short Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach
title_sort fluidity of the system produced in relativistic pp and heavy-ion collisions: hadron resonance gas model approach
topic nucl-th
Nuclear Physics - Theory
nucl-ex
Nuclear Physics - Experiment
hep-ex
Particle Physics - Experiment
hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1140/epja/s10050-023-01052-1
https://dx.doi.org/10.1140/epja/s10050-023-01052-1
http://cds.cern.ch/record/2800102
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AT sahudushmanta fluidityofthesystemproducedinrelativisticppandheavyioncollisionshadronresonancegasmodelapproach
AT singhcaptainr fluidityofthesystemproducedinrelativisticppandheavyioncollisionshadronresonancegasmodelapproach
AT sahooraghunath fluidityofthesystemproducedinrelativisticppandheavyioncollisionshadronresonancegasmodelapproach
AT alamjane fluidityofthesystemproducedinrelativisticppandheavyioncollisionshadronresonancegasmodelapproach