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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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 |
work_keys_str_mv |
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