The NJL model and strange quark matter
arXiv:hep-ph/0210295 · doi:10.1209/epl/i2003-00171-0
Abstract
The stability of strange quark matter is studied within the Nambu Jona-Lasinio model with three different parameter sets. The model Lagrangian contains 4-fermion (with and without vector interaction) and 6-fermion terms; the minimum energy per baryon number as a function of the strangeness fraction of the system is compared to the masses of hyperons having the same strangeness fraction, and coherently calculated in the same version of the model, and for the same parameter set. The results show that in none of the different parameter sets strangelets are stable, and in some cases a minimum in the energy per baryon does not even exist.
8 pages, 2 figures, reference added, typos corrected, version to appear in Europhys. Lett
Cited by in corpus (10)
- NJL-model analysis of dense quark matter
- Quark deconfinement in high-mass neutron stars
- Quark matter may not be strange
- Thermodynamics with density and temperature dependent particle masses and properties of bulk strange quark matter and strangelets
- Quark droplets stability induced by external magnetic field
- Unified Interacting Quark Matter and its Astrophysical Implications
- GW190814: Circumstantial Evidence for Up-Down Quark Star
- Magnetized quark matter with a magnetic-field dependent coupling
- Effects of the temperature and magnetic-field dependent coupling on the properties of QCD matter
- The compressibility of quark matter under strong magnetic field in the NJL model