Proceedings of XTH Quark Confinement and the Hadron Spectrum — PoS(Confinement X) 2013
DOI: 10.22323/1.171.0249
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Nonlocal PNJL models and quark matter in compact stars

Abstract: Nonlocal PNJL models allow for a detailed description of chiral quark dynamics with running quark masses and wave function renormalization in accordance with lattice QCD (LQCD) in vacuum. Their generalization to finite temperature T and chemical potential µ allows to reproduce the * Speaker.

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Cited by 36 publications
(56 citation statements)
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“…Fukushima & Sasaki 2013;Fukushima 2014). Since increasing the isospin asymmetry would result in lowering the temperature of the CEP to zero (Ohnishi et al 2011) the detection of first-order phase transition signals in zero temperature asymmetric compact star matter like the mass twin phenomenon would thus prove the existence of at least one CEP in the QCD phase diagram Alvarez-Castillo & Blaschke (2013), Blaschke et al (2013a). Unfortunately, heavy-ion collision experiments probe matter with only slight isospin asymmetry of about 60% neutron excess and hence cannot provide constraints for larger isospin asymmetry or even β-equilibrium (>90 % neutron excess) relevant for compact star phenomenology.…”
Section: Introductionmentioning
confidence: 98%
“…Fukushima & Sasaki 2013;Fukushima 2014). Since increasing the isospin asymmetry would result in lowering the temperature of the CEP to zero (Ohnishi et al 2011) the detection of first-order phase transition signals in zero temperature asymmetric compact star matter like the mass twin phenomenon would thus prove the existence of at least one CEP in the QCD phase diagram Alvarez-Castillo & Blaschke (2013), Blaschke et al (2013a). Unfortunately, heavy-ion collision experiments probe matter with only slight isospin asymmetry of about 60% neutron excess and hence cannot provide constraints for larger isospin asymmetry or even β-equilibrium (>90 % neutron excess) relevant for compact star phenomenology.…”
Section: Introductionmentioning
confidence: 98%
“…On the other hand, if the canonical 1.4M has a radius larger than about 14km, it implies that the hadronic equation of state is stiff at large densities and even the maximum mass configuration could be composed by just nucleon because its central density is smaller than the thresholds of hyperons and deltas. A phase transition to quark matter could still occur at large densities, as proposed in [59], leading to a third family branch of hybrid stars with masses close to 2M . Testing this scenario, which is very much different with respect to ours, would require precise measurements of the radii of the most massive stars.…”
Section: Icnfp 2014mentioning
confidence: 86%
“…This third family of CS is observationally detectable (in principle) by simultaneous mass and radius measurement with sufficient accuracy whereby the high masses should be about the same, such as for the two known high-mass pulsars PSR J1614-2230 [4] and PSR J0348+0432 [5] but the radii should differ, resulting in the "mass twin" phenomenon [37,38,39,40]. Also shown are previous models which could obtain the high mass twin phenomenon, see [12] for comparison. In the left panel of Fig.…”
Section: Advanced Njl Model For High-density Quark Mattermentioning
confidence: 99%
“…The answer is positive and leads to the characteristic feature of high-mass twin stars, see also [11,12]. In the following two sections we shall discuss the EVA and the density-dependent stiffening of quark matter in an advanced Nambu-Jona-Lasinio (NJL) model, respectively, both being the main ingredients to this new class of EoS for CS to be summarized in the subsequent section.…”
Section: Introductionmentioning
confidence: 99%