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Initial state fluctuations and the sub-leading flow modes from the experimental data and HYDJET++ model
A few microseconds after the birth of the Universe, the Universe was filled with the matter consisting of quarks and gluons, called quark gluon plasma (QGP). That primordial QGP lasts for about a few μ s until the Universe cooled down and expanded enough that colored quarks had to confine within the...
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Published in: | The European physical journal. D, Atomic, molecular, and optical physics Atomic, molecular, and optical physics, 2021, Vol.75 (1), Article 14 |
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description | A few microseconds after the birth of the Universe, the Universe was filled with the matter consisting of quarks and gluons, called quark gluon plasma (QGP). That primordial QGP lasts for about a few
μ
s
until the Universe cooled down and expanded enough that colored quarks had to confine within the colorless new formed hadrons. In high-energy nuclear collisions, where a high baryon density, or a high temperature could be achieved, small pieces of the QGP can be recreated and studied experimentally. Such created QGP undergoes an explosion, called the Little Bang. In spite of its small size (about 1000
f
m
3
) and short duration (a few
fm
/
c
, where
c
is the speed of light), the QGP is well described by relativistic hydrodynamics, including even the small perturbations on top of the explosion. In high-energy nucleus–nucleus (AA) collisions which have been performed at the Relativistic Heavy Ion Collider and at the Large Hadron Collider, the QGP was created with extremely high temperature and the baryon density close to zero. One of observables used to study QGP is azimuthal anisotropy. It was found that the initial state fluctuations have a significant influence on azimuthal anisotropies. We present results on azimuthal anisotropies measured in ultra-central PbPb collisions at
s
NN
= 2.76 TeV by the CMS and ALICE collaborations, as well as the leading and sub-leading flow modes for the elliptic and triangular anisotropies. The measured flow modes are also compared with the predictions from the HYDJET++ model.
Graphic abstract |
doi_str_mv | 10.1140/epjd/s10053-020-00037-9 |
format | article |
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μ
s
until the Universe cooled down and expanded enough that colored quarks had to confine within the colorless new formed hadrons. In high-energy nuclear collisions, where a high baryon density, or a high temperature could be achieved, small pieces of the QGP can be recreated and studied experimentally. Such created QGP undergoes an explosion, called the Little Bang. In spite of its small size (about 1000
f
m
3
) and short duration (a few
fm
/
c
, where
c
is the speed of light), the QGP is well described by relativistic hydrodynamics, including even the small perturbations on top of the explosion. In high-energy nucleus–nucleus (AA) collisions which have been performed at the Relativistic Heavy Ion Collider and at the Large Hadron Collider, the QGP was created with extremely high temperature and the baryon density close to zero. One of observables used to study QGP is azimuthal anisotropy. It was found that the initial state fluctuations have a significant influence on azimuthal anisotropies. We present results on azimuthal anisotropies measured in ultra-central PbPb collisions at
s
NN
= 2.76 TeV by the CMS and ALICE collaborations, as well as the leading and sub-leading flow modes for the elliptic and triangular anisotropies. The measured flow modes are also compared with the predictions from the HYDJET++ model.
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μ
s
until the Universe cooled down and expanded enough that colored quarks had to confine within the colorless new formed hadrons. In high-energy nuclear collisions, where a high baryon density, or a high temperature could be achieved, small pieces of the QGP can be recreated and studied experimentally. Such created QGP undergoes an explosion, called the Little Bang. In spite of its small size (about 1000
f
m
3
) and short duration (a few
fm
/
c
, where
c
is the speed of light), the QGP is well described by relativistic hydrodynamics, including even the small perturbations on top of the explosion. In high-energy nucleus–nucleus (AA) collisions which have been performed at the Relativistic Heavy Ion Collider and at the Large Hadron Collider, the QGP was created with extremely high temperature and the baryon density close to zero. One of observables used to study QGP is azimuthal anisotropy. It was found that the initial state fluctuations have a significant influence on azimuthal anisotropies. We present results on azimuthal anisotropies measured in ultra-central PbPb collisions at
s
NN
= 2.76 TeV by the CMS and ALICE collaborations, as well as the leading and sub-leading flow modes for the elliptic and triangular anisotropies. The measured flow modes are also compared with the predictions from the HYDJET++ model.
Graphic abstract</description><subject>Anisotropy</subject><subject>Applications of Nonlinear Dynamics and Chaos Theory</subject><subject>Atomic</subject><subject>Atomic collisions</subject><subject>Baryons</subject><subject>Computational fluid dynamics</subject><subject>Density</subject><subject>Fluid flow</subject><subject>Gluons</subject><subject>Hadrons</subject><subject>Heavy ions</subject><subject>High temperature</subject><subject>Hydrodynamics</subject><subject>Large Hadron Collider</subject><subject>Molecular</subject><subject>Optical and Plasma Physics</subject><subject>Physical Chemistry</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Information Technology</subject><subject>Quantum Physics</subject><subject>Quark-gluon plasma</subject><subject>Quarks</subject><subject>Regular Article - Topical Issue</subject><subject>Relativistic effects</subject><subject>Relativistic Heavy Ion Collider</subject><subject>Solenoids</subject><subject>Spectroscopy/Spectrometry</subject><subject>Spintronics</subject><subject>Topical Issue: Advances in Physics of Ionized Gases and Spectroscopy of Isolated Complex Systems: from Biomolecules to Space Particles - SPIG 2020</subject><subject>Universe</subject><issn>1434-6060</issn><issn>1434-6079</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNqFkEFLwzAYhoMoOKe_wYLHEZc0adMcZW5uMvCyi6eQtl9mR9fWJEX992at6NFTPsjzvN_Hi9AtJfeUcjKH7lDOHSUkYZjEBBNCmMDyDE0oZxynRMjz3zkll-jKuUOA4oSnE7TfNJWvdB05rz1Epu4L32tftY2LdFNG_g0i1-e4Bl1WzT4A7Ud0bEtwkbHtcfiHzw5sdYTGh5xSez2Y69fH5-VuNhvo-hpdGF07uPl5p2i3Wu4Wa7x9edosHra4oDKROJcSQJKkSDKjtSm4EZxTlifAWVECoZRlXINhImcpo1pmjElBCq1jMDFjU3Q3xna2fe_BeXVoe9uEjSrmQsQpTzMeKDFShW2ds2BUF-7X9ktRok6lqlOpaixVhVLVUKqSwcxG0wWj2YP9y_9P_QYInH3S</recordid><startdate>2021</startdate><enddate>2021</enddate><creator>Milosevic, J.</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>2021</creationdate><title>Initial state fluctuations and the sub-leading flow modes from the experimental data and HYDJET++ model</title><author>Milosevic, J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1959-b99ee905c58faafc4f74413b5e43cde011384aef37b3631a9833970caa2ef233</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Anisotropy</topic><topic>Applications of Nonlinear Dynamics and Chaos Theory</topic><topic>Atomic</topic><topic>Atomic collisions</topic><topic>Baryons</topic><topic>Computational fluid dynamics</topic><topic>Density</topic><topic>Fluid flow</topic><topic>Gluons</topic><topic>Hadrons</topic><topic>Heavy ions</topic><topic>High temperature</topic><topic>Hydrodynamics</topic><topic>Large Hadron Collider</topic><topic>Molecular</topic><topic>Optical and Plasma Physics</topic><topic>Physical Chemistry</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Information Technology</topic><topic>Quantum Physics</topic><topic>Quark-gluon plasma</topic><topic>Quarks</topic><topic>Regular Article - Topical Issue</topic><topic>Relativistic effects</topic><topic>Relativistic Heavy Ion Collider</topic><topic>Solenoids</topic><topic>Spectroscopy/Spectrometry</topic><topic>Spintronics</topic><topic>Topical Issue: Advances in Physics of Ionized Gases and Spectroscopy of Isolated Complex Systems: from Biomolecules to Space Particles - SPIG 2020</topic><topic>Universe</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Milosevic, J.</creatorcontrib><collection>CrossRef</collection><jtitle>The European physical journal. D, Atomic, molecular, and optical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Milosevic, J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Initial state fluctuations and the sub-leading flow modes from the experimental data and HYDJET++ model</atitle><jtitle>The European physical journal. D, Atomic, molecular, and optical physics</jtitle><stitle>Eur. Phys. J. D</stitle><date>2021</date><risdate>2021</risdate><volume>75</volume><issue>1</issue><artnum>14</artnum><issn>1434-6060</issn><eissn>1434-6079</eissn><abstract>A few microseconds after the birth of the Universe, the Universe was filled with the matter consisting of quarks and gluons, called quark gluon plasma (QGP). That primordial QGP lasts for about a few
μ
s
until the Universe cooled down and expanded enough that colored quarks had to confine within the colorless new formed hadrons. In high-energy nuclear collisions, where a high baryon density, or a high temperature could be achieved, small pieces of the QGP can be recreated and studied experimentally. Such created QGP undergoes an explosion, called the Little Bang. In spite of its small size (about 1000
f
m
3
) and short duration (a few
fm
/
c
, where
c
is the speed of light), the QGP is well described by relativistic hydrodynamics, including even the small perturbations on top of the explosion. In high-energy nucleus–nucleus (AA) collisions which have been performed at the Relativistic Heavy Ion Collider and at the Large Hadron Collider, the QGP was created with extremely high temperature and the baryon density close to zero. One of observables used to study QGP is azimuthal anisotropy. It was found that the initial state fluctuations have a significant influence on azimuthal anisotropies. We present results on azimuthal anisotropies measured in ultra-central PbPb collisions at
s
NN
= 2.76 TeV by the CMS and ALICE collaborations, as well as the leading and sub-leading flow modes for the elliptic and triangular anisotropies. The measured flow modes are also compared with the predictions from the HYDJET++ model.
Graphic abstract</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1140/epjd/s10053-020-00037-9</doi></addata></record> |
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subjects | Anisotropy Applications of Nonlinear Dynamics and Chaos Theory Atomic Atomic collisions Baryons Computational fluid dynamics Density Fluid flow Gluons Hadrons Heavy ions High temperature Hydrodynamics Large Hadron Collider Molecular Optical and Plasma Physics Physical Chemistry Physics Physics and Astronomy Quantum Information Technology Quantum Physics Quark-gluon plasma Quarks Regular Article - Topical Issue Relativistic effects Relativistic Heavy Ion Collider Solenoids Spectroscopy/Spectrometry Spintronics Topical Issue: Advances in Physics of Ionized Gases and Spectroscopy of Isolated Complex Systems: from Biomolecules to Space Particles - SPIG 2020 Universe |
title | Initial state fluctuations and the sub-leading flow modes from the experimental data and HYDJET++ model |
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