Abstract
We study what happens to the Nucleon, Delta and Omega 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 Nf=2+1 ensembles, with four temperatures below and four above the deconfinement transition temperature. Below Tc 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 Tc we find a clear signal of parity doubling in all three channels, with the effect of the heavier s quark visible.
Original language | English |
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Article number | 34 |
Journal | Journal of High Energy Physics |
Volume | 2017 |
Issue number | 6 |
ISSN | 1126-6708 |
DOIs | |
Publication status | Published - 27. Mar 2017 |
Bibliographical note
33 pages, several figures; additional evidence on the absence of light baryonic bound states in the QGP provided, references added, to appear in JHEPKeywords
- Lattice Quantum Field Theory
- Phase Diagram of QCD
- Quark-Gluon Plasma
- Thermal Field Theory