1998
DOI: 10.1016/s0370-2693(98)00935-6
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Strange stars with realistic quark vector interaction and phenomenological density-dependent scalar potential

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Cited by 328 publications
(387 citation statements)
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“…In this model the quark interaction is described by an interquark vector potential originating from gluon exchange and by a density-dependent scalar potential that restores the chiral symmetry at high density. Using the same model (with the parameterization [Dey et al 1998, erratum] denoted as SS1 and SS2), 8 we calculated the M-R relations, which are also shown by solid curves labeled SS1 and SS2 in Figure 1, corresponding to strange stars with maximum masses of 1.44 and 1.32 M , and radii of 7.07 and 6.53 7 There are actually two solutions of eq. (7) with given I and M; one serves as the upper limit of R and the other the lower limit of R. But the former solution gives an unphysically small radius and is rejected.…”
Section: The Mass-radius Relation For 4u 1728ϫ34mentioning
confidence: 99%
See 1 more Smart Citation
“…In this model the quark interaction is described by an interquark vector potential originating from gluon exchange and by a density-dependent scalar potential that restores the chiral symmetry at high density. Using the same model (with the parameterization [Dey et al 1998, erratum] denoted as SS1 and SS2), 8 we calculated the M-R relations, which are also shown by solid curves labeled SS1 and SS2 in Figure 1, corresponding to strange stars with maximum masses of 1.44 and 1.32 M , and radii of 7.07 and 6.53 7 There are actually two solutions of eq. (7) with given I and M; one serves as the upper limit of R and the other the lower limit of R. But the former solution gives an unphysically small radius and is rejected.…”
Section: The Mass-radius Relation For 4u 1728ϫ34mentioning
confidence: 99%
“…Recently, Dey et al (1998) derived an EOS for strange matter that has asymptotic freedom built in, shows confinement at zero baryon density and deconfinement at high density, and gives a stable configuration for chargeless, b-stable strange matter. In this model the quark interaction is described by an interquark vector potential originating from gluon exchange and by a density-dependent scalar potential that restores the chiral symmetry at high density.…”
Section: The Mass-radius Relation For 4u 1728ϫ34mentioning
confidence: 99%
“…The two curves SSI and SS2 in Fig. 1 give the MR relation for strange stars calculated with the EOS by Dey et al (1998). Figure 1 clearly demonstrates that a strange star model is more compatible with SAX J 1808.4-3658 than a neutron star one.…”
Section: Strange Star Candidatesmentioning
confidence: 74%
“…4-3658 (Li et al 1999a), the atoll X-ray source 4U 1728-34 (Li et al 1999b), the X-ray burster 4U 1820-30 (Bombaci 1997), the X-ray pulsar Her X-l (Dey et al 1998), and the hard X-ray burster GRO J1744-28 (Cheng et al 1998) are good strange star candidates. If the compact objects in these X-ray sources are really strange stars, then there will be very deep consequences for both astrophysics and the physics of strong interactions.…”
Section: Strange Star Candidatesmentioning
confidence: 99%
“…Equations of state N1, N2, and PC are not modern (i.e., not fitted to the most current nuclear scattering data), but are included for easy comparison to previous work on equation of state constraints. Curve S1 is for a compact strange star (Dey et al 1998), whereas curve S2 is for a more standard strange star equation of state (Zdunik 2000). Curve Q is a quark matter equation of state with a Gaussian form factor and a diquark condensate (kindly provided by David Blaschke and Hovik Gregorian).…”
Section: Results: Vela X-1mentioning
confidence: 99%