Light baryons below and above the deconfinement transition: medium effects and parity doubling

Abstract We study what happens to the N , Δ and Ω baryons in the hadronic gas and the quark-gluon plasma, with particular interest in parity doubling and its emergence as the plasma is heated. This is done using simulations of lattice QCD, employing the FASTSUM anisotropic N f = 2 + 1 ensembles, wit...

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Main Authors: Gert Aarts, Chris Allton, Davide De Boni, Simon Hands, Benjamin Jäger, Chrisanthi Praki, Jon-Ivar Skullerud
Format: Article
Language:English
Published: SpringerOpen 2017-06-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP06(2017)034
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spelling doaj-6f0ee020186240919dc5166708fa88052020-11-24T20:57:14ZengSpringerOpenJournal of High Energy Physics1029-84792017-06-012017613010.1007/JHEP06(2017)034Light baryons below and above the deconfinement transition: medium effects and parity doublingGert Aarts0Chris Allton1Davide De Boni2Simon Hands3Benjamin Jäger4Chrisanthi Praki5Jon-Ivar Skullerud6Department of Physics, College of Science, Swansea UniversityDepartment of Physics, College of Science, Swansea UniversityDepartment of Physics, College of Science, Swansea UniversityDepartment of Physics, College of Science, Swansea UniversityDepartment of Physics, College of Science, Swansea UniversityDepartment of Physics, College of Science, Swansea UniversityDepartment of Theoretical Physics, |National University of Ireland MaynoothAbstract We study what happens to the N , Δ and Ω baryons in the hadronic gas and the quark-gluon plasma, with particular interest in parity doubling and its emergence as the plasma is heated. This is done using simulations of lattice QCD, employing the FASTSUM anisotropic N f = 2 + 1 ensembles, with four temperatures below and four above the deconfinement transition temperature. Below T c we find that the positive-parity groundstate masses are largely temperature independent, whereas the negative-parity ones are reduced considerably as the temperature increases. This may be of interest for heavy-ion phenomenology. Close to the transition, the masses are nearly degenerate, in line with the expectation from chiral symmetry restoration. Above T c we find a clear signal of parity doubling in all three channels, with the effect of the heavier s quark visible.http://link.springer.com/article/10.1007/JHEP06(2017)034Lattice Quantum Field TheoryPhase Diagram of QCDQuark-Gluon PlasmaThermal Field Theory
collection DOAJ
language English
format Article
sources DOAJ
author Gert Aarts
Chris Allton
Davide De Boni
Simon Hands
Benjamin Jäger
Chrisanthi Praki
Jon-Ivar Skullerud
spellingShingle Gert Aarts
Chris Allton
Davide De Boni
Simon Hands
Benjamin Jäger
Chrisanthi Praki
Jon-Ivar Skullerud
Light baryons below and above the deconfinement transition: medium effects and parity doubling
Journal of High Energy Physics
Lattice Quantum Field Theory
Phase Diagram of QCD
Quark-Gluon Plasma
Thermal Field Theory
author_facet Gert Aarts
Chris Allton
Davide De Boni
Simon Hands
Benjamin Jäger
Chrisanthi Praki
Jon-Ivar Skullerud
author_sort Gert Aarts
title Light baryons below and above the deconfinement transition: medium effects and parity doubling
title_short Light baryons below and above the deconfinement transition: medium effects and parity doubling
title_full Light baryons below and above the deconfinement transition: medium effects and parity doubling
title_fullStr Light baryons below and above the deconfinement transition: medium effects and parity doubling
title_full_unstemmed Light baryons below and above the deconfinement transition: medium effects and parity doubling
title_sort light baryons below and above the deconfinement transition: medium effects and parity doubling
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2017-06-01
description Abstract We study what happens to the N , Δ and Ω baryons in the hadronic gas and the quark-gluon plasma, with particular interest in parity doubling and its emergence as the plasma is heated. This is done using simulations of lattice QCD, employing the FASTSUM anisotropic N f = 2 + 1 ensembles, with four temperatures below and four above the deconfinement transition temperature. Below T c we find that the positive-parity groundstate masses are largely temperature independent, whereas the negative-parity ones are reduced considerably as the temperature increases. This may be of interest for heavy-ion phenomenology. Close to the transition, the masses are nearly degenerate, in line with the expectation from chiral symmetry restoration. Above T c we find a clear signal of parity doubling in all three channels, with the effect of the heavier s quark visible.
topic Lattice Quantum Field Theory
Phase Diagram of QCD
Quark-Gluon Plasma
Thermal Field Theory
url http://link.springer.com/article/10.1007/JHEP06(2017)034
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