Hot hybrid neutron star matter within a statistical baryonic approach and the PNJL quark model

被引:0
作者
Ghaemmaghami, S. A. [1 ]
Mojarrad, M. Ghazanfari [1 ]
机构
[1] Univ Kashan, Fac Sci, Dept Phys, POB 87317-53153, Kashan, Iran
基金
美国国家科学基金会;
关键词
EQUATION-OF-STATE; FINITE-TEMPERATURE; NUCLEAR-MATTER; DENSE MATTER; APPROXIMATION; SIMULATIONS; SUPERNOVAE; NICER; MASS;
D O I
10.1103/PhysRevD.111.023026
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Due to the lack of a universally accepted model for determining the structure and composition of a hot hybrid neutron star (HHNS), continuous efforts are being made to improve the existing models. Thus, in this study, we set out to model HHNSs by utilizing a statistical model based on Thomas-Fermi approximation for baryonic matter, and the Polyakov-Nambu-Jona-Lasino model for quark matter to describe the baryon-quark phase transition using the Maxwell construction for neutrino-free matter and neutrino-trapped matter under the beta equilibrium conditions, while adopting the isothermal (isentropic) equation of state (EOS) of baryonic matter with the interactions MS96 and MS90, and the one of quark matter where the quark vector interactions are included. According to our research findings, besides the repulsive effects arising from the baryonic interactions in phase space, and the quark vector couplings, it is concluded that the temperature and neutrino trapping significantly affect the stiffness of the hot hybrid EOS. Within the isentropic picture, the EOS of neutrino-free matter turns out to be more sensitive to the value of the entropy per baryon than that of neutrino-trapped matter. Additionally, with an increase in entropy per baryon, the HHNS structures with larger gravitational (baryonic) masses are allowed, while the ones with smaller radii are excluded. Most importantly, our calculations show that the possibility of obtaining a stable mass structure of HHNSs cannot be excluded under the conditions of quark vector interaction and neutrino trapping.
引用
收藏
页数:19
相关论文
共 93 条
[1]  
Abbott R., 2020, Astrophys. J. Lett., V896, pL44
[2]   Equation of state of nucleon matter and neutron star structure [J].
Akmal, A ;
Pandharipande, VR ;
Ravenhall, DG .
PHYSICAL REVIEW C, 1998, 58 (03) :1804-1828
[3]   High density symmetric nuclear matter in the Bethe-Brueckner-Goldstone approach [J].
Baldo, M ;
Fiasconaro, A ;
Song, HQ ;
Giansiracusa, G ;
Lombardo, U .
PHYSICAL REVIEW C, 2002, 65 (01) :173031-173034
[4]   THERMOSTATIC PROPERTIES OF FINITE AND INFINITE NUCLEAR SYSTEMS [J].
BANDYOPADHYAY, D ;
SAMANTA, C ;
SAMADDAR, SK ;
DE, JN .
NUCLEAR PHYSICS A, 1990, 511 (01) :1-28
[5]   ENERGY-DEPENDENT POTENTIAL IN NUCLEAR COLLISIONS [J].
BANDYOPADHYAY, D ;
SAMADDAR, SK .
NUCLEAR PHYSICS A, 1988, 484 (02) :315-336
[6]   Nuclear incompressibility using the density-dependent M3Y effective interaction [J].
Basu, DN .
JOURNAL OF PHYSICS G-NUCLEAR AND PARTICLE PHYSICS, 2004, 30 (06) :B7-B11
[7]   Effects of quark matter nucleation on the evolution of proto-neutron stars [J].
Bombaci, I. ;
Logoteta, D. ;
Providencia, C. ;
Vidana, I. .
ASTRONOMY & ASTROPHYSICS, 2011, 528
[8]   Role of vector interaction and axial anomaly in the PNJL modeling of the QCD phase diagram [J].
Bratovic, Nino ;
Hatsuda, Tetsuo ;
Weise, Wolfram .
PHYSICS LETTERS B, 2013, 719 (1-3) :131-135
[9]   NJL-model analysis of dense quark matter [J].
Buballa, M .
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 2005, 407 (4-6) :205-376
[10]  
Camenzind M., 2007, Compact Objects in Astrophysics: White Dwarfs, Neutron Stars, and Black Holes