2020
DOI: 10.1103/physrevd.102.083030
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Quark matter in light neutron stars

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Cited by 37 publications
(41 citation statements)
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References 72 publications
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“…7), astronomical observations can also be used to place constraints on the relevant parameter space. In general, since GW170817 provided an upper limit onΛ, any physical effect that results in a softening of the equation of state can be consistent with the data [88,[240][241][242][243][244][245][246] As such, a strong first-order phase transition might make an equation of state model compatible with the GW170817 data, even if the hadronic part on its own is not [152,[247][248][249][250]. A number of studies have constructed models that can successfully interpret the inspiral signal from GW170817 as the coalescence of any combination of hadronic and hybrid hadronic-quark neutron stars and place corresponding constraints on the relevant model parameter space [149,247,248,[251][252][253][254][255][256][257][258][259][260].…”
Section: Microscopic Propertiesmentioning
confidence: 85%
“…7), astronomical observations can also be used to place constraints on the relevant parameter space. In general, since GW170817 provided an upper limit onΛ, any physical effect that results in a softening of the equation of state can be consistent with the data [88,[240][241][242][243][244][245][246] As such, a strong first-order phase transition might make an equation of state model compatible with the GW170817 data, even if the hadronic part on its own is not [152,[247][248][249][250]. A number of studies have constructed models that can successfully interpret the inspiral signal from GW170817 as the coalescence of any combination of hadronic and hybrid hadronic-quark neutron stars and place corresponding constraints on the relevant model parameter space [149,247,248,[251][252][253][254][255][256][257][258][259][260].…”
Section: Microscopic Propertiesmentioning
confidence: 85%
“…In our previous works [49,50], we have analyzed hybrid stars using the NJL model with different interaction terms at the Lagrangian level which describes the quark phase. The usual three-flavor NJL model [20,51] with additional vector and pseudovector interactions and the vector-isovector and pseudovector-isovector interactions were explored in [49].…”
Section: Introductionmentioning
confidence: 99%
“…It was shown that considerable quark core sizes would require moderate values for the quark vector-isoscalar term and a weak vector isovector term. Additional higher-order repulsive interactions, four-quark and eight-quark vector-isoscalar interactions, were included in [50]. The eight-quark vector-isoscalar channel was shown to allow for the appearance of a quark core at moderately low NS masses, ∼1 M ⊙ , while providing the required repulsion to keep the star stability up to ∼2.1 M ⊙ .…”
Section: Introductionmentioning
confidence: 99%
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“…Indeed, even if the exact location of the deconfinement transition towards quark matter is essentially unknown, if strange quark matter is not absolutely stable such a transition is expected at high density [18]. In particular, if this transition is strongly first order, the parameter space of the EoS increases, leading to a much larger spread of the possible M(R) relation ( [19] and references therein). Because of the phenomenological nature of the effective models used for the quark phase, settling the parameter space associated to a phase transition to quark matter is a very hard task.…”
Section: Modelling the Neutron-star Equation Of Statementioning
confidence: 99%