Nuclear equation of state and finite nucleon volumes
arXiv:1501.06945 · doi:10.1088/0954-3899/42/4/045109
Abstract
It is shown how the Equation of State (EoS) depends on nucleon properties inside Nuclear Matter (NM). We propose to benefit from the concept of enthalpy in order to include volume corrections to the nucleon rest energy, which are proportional to pressure and absent in a standard Relativistic Mean Field (RMF) with point-like nucleons. As a result, the nucleon mass can decrease inside NM, making the model nonlinear and the EoS softer. The course of the EoS in our RMF model agrees with a semi-empirical estimate and is close to the results obtained from extensive DBHF calculations with a Bonn A potential, which produce an EoS stiff enough to describe neutron star properties (mass--radius constraint), especially the masses of PSR J1614_2230 and PSR J0348_0432, known as the most massive () neutron stars. The presented model has proper saturation properties, including a good value of compressibility.
12 pages,3 figures. Accepted in Journal of Physics G; Nuclear and Particle Physics. arXiv admin note: substantial text overlap with arXiv:1311.3591
References in corpus (12)
- Shapiro delay measurement of a two solar mass neutron star
- A Massive Pulsar in a Compact Relativistic Binary
- Constraints on the high-density nuclear equation of state from the phenomenology of compact stars and heavy-ion collisions
- Short Range Correlations and the EMC Effect
- Incompressibility in finite nuclei and nuclear matter
- Relativistic model for nuclear matter and atomic nuclei with momentum-dependent self-energies
- Modern compact star observations and the quark matter equation of state
- Pseudo-spin symmetry in density-dependent relativistic Hartree-Fock theory
- Crossover transition in bag-like models
- Recent progress constraining the nuclear equation of state from astrophysics and heavy ion reactions
- Constraining relativistic models through heavy ion collisions
- Compact Stars, Heavy Ion Collisions, and Possible Lessons For QCD at Finite Densities