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Quark 1.14
Quark 1.14




quark 1.14 quark 1.14

However, for the mass and radius given by Miller et al., no such parameter space exist. through the analysis of observational data of NICER, there exists a very tiny allowed parameter space for which strange stars computed for the QMDD model agree with the observations of PSR J 0740 + 6620, GW170817 and PSR J 0030 + 0451 simultaneously. We also find that for the mass and radius of PSR J 0030 + 0451 given by Riley et al. It is found that the largest possible maximum mass of a strange star obtained with the QMDD model is 2.42 M ⊙ and that the secondary component of GW190814 with a mass of 2.59 − 0.09 + 0.08 M ⊙ could not be a static strange star.

quark 1.14

For the current quark masses of m u 0 = 2.16 MeV, m d 0 = 4.67 MeV, and m s 0 = 93 MeV, we find that a strange star can exist for values of the non-Newtonian gravity parameter g 2 / μ 2 in the range of 4.58 GeV − 2 ≤ g 2 / μ 2 ≤ 9.32 GeV − 2, and that the parameters D and C of the QMDD model are restricted to 158.3 MeV ≤ D 1 / 2 ≤ 181.2 MeV and − 0.65 ≤ C ≤ − 0.12. We find that for the QMDD model these mass and tidal deformability observations would rule out the existence of strange stars if non-Newtonian gravity effects are ignored. Using a density dependent quark mass (QMDD) model for strange quark matter, we investigate the effects of non-Newtonian gravity on the properties of strange stars and constrain the parameters of the QMDD model by employing the mass of PSR J 0740 + 6620 and the tidal deformability of GW170817.






Quark 1.14