Anisotropic star in Vaidya-Tikekar model admitting MIT bag model equation of state in pseudo-spheroidal geometry

2021 ◽  
Vol 366 (10) ◽  
Author(s):  
A. Saha ◽  
K. B. Goswami ◽  
P. K. Chattopadhyay
2007 ◽  
Vol 22 (14) ◽  
pp. 1019-1029 ◽  
Author(s):  
ABHIJIT BHATTACHARYYA ◽  
SANJAY K. GHOSH

The properties of rotating quark star are studied using the equation of state obtained from chiral colour dielectric model. The results are compared with those obtained from MIT bag model equation of state. The frequencies in the corotating innermost circular orbits for different central densities are evaluated and compared with the observed data.


2010 ◽  
Vol 692 (4) ◽  
pp. 277-280 ◽  
Author(s):  
Sz. Horvát ◽  
V.K. Magas ◽  
D.D. Strottman ◽  
L.P. Csernai

2003 ◽  
Vol 12 (03) ◽  
pp. 495-507 ◽  
Author(s):  
G. LUGONES ◽  
J. E. HORVATH

We present the equation of state (EOS) of quark-diquark matter in the quark mass-density-dependent model. The region of the 2-D parameter space inside which this quark-diquark matter is stable against diquark disassembling and hadronization is determined. Motivated by observational data suggesting a high compactness of some neutron stars (NS) we present models based on the present EOS and compare the results with those obtained with previous works addressing a quark-diquark composition based on the MIT Bag model. We show that very compact self-bound stars (yet having ≥ 1M⊙) are allowed by our EOS even if the diquark itself is unbound.


1998 ◽  
Vol 07 (01) ◽  
pp. 29-48 ◽  
Author(s):  
O. G. BENVENUTO ◽  
G. LUGONES

We study the general properties of compact objects made up of strange matter in the framework of a new equation of state in which the quark masses are parametrized as functions of the baryon density, so that they are heavy (light) at low (high) densities. This has been called the "quark mass-density-dependent model." In this approximation, the strange matter equation of state is rather similar to the corresponding to the MIT Bag Model, but it is significantly stiffer at low densities. Such a property modifies the structure of strange stars in a sizeable way. In this framework, we calculate the structure of strange stars (mass, radius, central density, gravitational redshift, moment of inertia, and total baryon number) finding that the resulting structures are rather similar to those obtained in the MIT Bag model, although some important differences appear. Comparing to the standard bagged case (with a bag constant in the range of B = 60 - 80 MeV fm-3), we find that these objects may be more massive and may show gravitational redshifts larger (up to ≈ 10%) than in the bag case. The moment of inertia and total baryon number may be larger than in the bagged case up to a factor of three. We also calculate the first three radial pulsation modes of these objects, finding that the relation of period vs. gravitational redshift is rather similar to the bag case. Also, we present an analytical treatment for such modes in the low-mass strange stars regime, which is in reasonable agreement with the numerical results.


2006 ◽  
Vol 21 (28n29) ◽  
pp. 5991-6001 ◽  
Author(s):  
G. H. BORDBAR ◽  
M. BIGDELI ◽  
T. YAZDIZADEH

The equation of state of deconfined quark matter within the MIT bag model is calculated. This equation of state is used to compute the structure of a neutron star with quark core. It is found that the limiting mass of the neutron star is affected considerably by this modification of the equation of state. Calculations are carried out for different choices of the bag constant.


2011 ◽  
Vol 20 (08) ◽  
pp. 1805-1815 ◽  
Author(s):  
V. V. BEGUN ◽  
M. I. GORENSTEIN ◽  
O. A. MOGILEVSKY

The modified versions of the bag model equation of state (EoS) are considered. They are constructed to satisfy the main qualitative features observed for the quark–gluon plasma EoS in the lattice QCD calculations. A quantitative comparison with the lattice results at high temperatures T are done in the SU(3) gluodynamics and in the full QCD with dynamical quarks. Our analysis advocates a negative value of the bag constant B.


Author(s):  
Salil Joshi ◽  
Sovan Sau ◽  
Soma Sanyal
Keyword(s):  

1983 ◽  
Vol 27 (11) ◽  
pp. 2708-2714 ◽  
Author(s):  
P. J. Mulders ◽  
G. Bhamathi ◽  
L. Heller ◽  
A. T. Aerts ◽  
A. K. Kerman
Keyword(s):  

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