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Charming Charm, Beautiful Bottom, and Quark-Gluon Plasma in the Large Hadron Collider Era
After a few microseconds of the creation of our Universe through the Big Bang, the primordial matter was believed to be a soup of the fundamental constituents of matter -- quarks and gluons. This is expected to be created in the laboratory by colliding heavy nuclei at ultra-relativistic speeds. A pl...
Autores principales: | , |
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Lenguaje: | eng |
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2021
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.18520/cs/v121/i9/1156-1161 http://cds.cern.ch/record/2790823 |
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author | Das, Santosh K. Sahoo, Raghunath |
author_facet | Das, Santosh K. Sahoo, Raghunath |
author_sort | Das, Santosh K. |
collection | CERN |
description | After a few microseconds of the creation of our Universe through the Big Bang, the primordial matter was believed to be a soup of the fundamental constituents of matter -- quarks and gluons. This is expected to be created in the laboratory by colliding heavy nuclei at ultra-relativistic speeds. A plasma of quarks and gluons, called Quark-Gluon Plasma (QGP) can be created at the energy and luminosity frontiers in the Relativistic Heavy Ion Collider (RHIC), at Brookhaven National Laboratory, New York, USA, and the Large Hadron Collider (LHC) at CERN, Geneva, Switzerland. Heavy quarks, namely the charm and bottom quarks, are considered as novel probes to characterize QGP, and hence the produced Quantum Chromodynamics (QCD) matter. Heavy quark transport coefficients play a significant role in understanding the properties of QGP. Experimental measurements of nuclear suppression factor and elliptic flow can constrain the heavy quark transport coefficients, which are key ingredients for phenomenological studies, and they help to disentangle different energy loss mechanisms. We give a general perspective of the heavy quark drag and diffusion coefficients in QGP and discuss their potentials as probes to disentangle different hadronization mechanisms, as well as to probe the initial electromagnetic fields produced in non-central heavy-ion collisions. Experimental perspectives on future measurements are discussed with special emphasis on heavy-flavors as next-generation probes in view of new technological developments. |
id | cern-2790823 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2021 |
record_format | invenio |
spelling | cern-27908232023-01-31T03:58:17Zdoi:10.18520/cs/v121/i9/1156-1161http://cds.cern.ch/record/2790823engDas, Santosh K.Sahoo, RaghunathCharming Charm, Beautiful Bottom, and Quark-Gluon Plasma in the Large Hadron Collider Eranucl-thNuclear Physics - Theorynucl-exNuclear Physics - Experimenthep-exParticle Physics - Experimenthep-phParticle Physics - PhenomenologyAfter a few microseconds of the creation of our Universe through the Big Bang, the primordial matter was believed to be a soup of the fundamental constituents of matter -- quarks and gluons. This is expected to be created in the laboratory by colliding heavy nuclei at ultra-relativistic speeds. A plasma of quarks and gluons, called Quark-Gluon Plasma (QGP) can be created at the energy and luminosity frontiers in the Relativistic Heavy Ion Collider (RHIC), at Brookhaven National Laboratory, New York, USA, and the Large Hadron Collider (LHC) at CERN, Geneva, Switzerland. Heavy quarks, namely the charm and bottom quarks, are considered as novel probes to characterize QGP, and hence the produced Quantum Chromodynamics (QCD) matter. Heavy quark transport coefficients play a significant role in understanding the properties of QGP. Experimental measurements of nuclear suppression factor and elliptic flow can constrain the heavy quark transport coefficients, which are key ingredients for phenomenological studies, and they help to disentangle different energy loss mechanisms. We give a general perspective of the heavy quark drag and diffusion coefficients in QGP and discuss their potentials as probes to disentangle different hadronization mechanisms, as well as to probe the initial electromagnetic fields produced in non-central heavy-ion collisions. Experimental perspectives on future measurements are discussed with special emphasis on heavy-flavors as next-generation probes in view of new technological developments.arXiv:2103.05551oai:cds.cern.ch:27908232021-03-09 |
spellingShingle | nucl-th Nuclear Physics - Theory nucl-ex Nuclear Physics - Experiment hep-ex Particle Physics - Experiment hep-ph Particle Physics - Phenomenology Das, Santosh K. Sahoo, Raghunath Charming Charm, Beautiful Bottom, and Quark-Gluon Plasma in the Large Hadron Collider Era |
title | Charming Charm, Beautiful Bottom, and Quark-Gluon Plasma in the Large Hadron Collider Era |
title_full | Charming Charm, Beautiful Bottom, and Quark-Gluon Plasma in the Large Hadron Collider Era |
title_fullStr | Charming Charm, Beautiful Bottom, and Quark-Gluon Plasma in the Large Hadron Collider Era |
title_full_unstemmed | Charming Charm, Beautiful Bottom, and Quark-Gluon Plasma in the Large Hadron Collider Era |
title_short | Charming Charm, Beautiful Bottom, and Quark-Gluon Plasma in the Large Hadron Collider Era |
title_sort | charming charm, beautiful bottom, and quark-gluon plasma in the large hadron collider era |
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/10.18520/cs/v121/i9/1156-1161 http://cds.cern.ch/record/2790823 |
work_keys_str_mv | AT dassantoshk charmingcharmbeautifulbottomandquarkgluonplasmainthelargehadroncolliderera AT sahooraghunath charmingcharmbeautifulbottomandquarkgluonplasmainthelargehadroncolliderera |