2021
DOI: 10.48550/arxiv.2104.05950
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Heavy Magnetic Neutron Stars

I. A. Rather,
Usuf Rahaman,
V. Dexheimer
et al.

Abstract: Context.Aims. We systematically study the properties of pure nucleonic and hyperonic magnetic stars using a density-dependent relativistic mean field (DD-RMF) equations of state. Methods. We explore several parameter sets and hyperon coupling schemes within the DD-RMF formalism. We focus on sets that agree with nuclear and other astrophysical data, while generating heavy neutron stars. Magnetic field effects are included in the matter equation of state and in general relativity solutions, which in addition ful… Show more

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Cited by 4 publications
(4 citation statements)
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“…A major challenge for realistic but still standard neutron star EoS models is producing a large maximum mass. Reaching masses as high as that of the light component of the GW190814 event is very difficult, specially when including hyperonic degrees of freedom (without resorting to fast rotation [11,12,16,23,[129][130][131][132], or strong magnetic fields [133]). Reaching masses as high as the companion of V723 Mon would not be possible at all with most standard EoS models.…”
Section: B How To Construct the Heaviest Neutron Starsmentioning
confidence: 99%
“…A major challenge for realistic but still standard neutron star EoS models is producing a large maximum mass. Reaching masses as high as that of the light component of the GW190814 event is very difficult, specially when including hyperonic degrees of freedom (without resorting to fast rotation [11,12,16,23,[129][130][131][132], or strong magnetic fields [133]). Reaching masses as high as the companion of V723 Mon would not be possible at all with most standard EoS models.…”
Section: B How To Construct the Heaviest Neutron Starsmentioning
confidence: 99%
“…A major challenge for realistic but still standard neutron star EoS models is producing a large maximum mass. Reaching masses as high as that of the light component of the GW190814 event is very difficult, specially when including hyperonic degrees of freedom (without resorting to fast rotation [11,12,16,23,[125][126][127][128], or strong magnetic fields [129]). Reaching masses as high as the companion of V723 Mon would not be possible at all with most standard EoS models.…”
Section: B How To Construct the Heaviest Neutron Starsmentioning
confidence: 99%
“…On the other hand, the possibility for GW190814's secondary as a neutron star can be accomplished by: 1) Choose/construct stiff EOSs having the maximum mass larger than 2.5 M [131][132][133][134][135][136][137][138][139][140][141] ; 2) Consider effects of fast rotations which can increases the maximum mass by about 20% when a star rotates at the Kepler frequency (the maximum frequency at which the gravitational attraction is still sufficient to keep matter bound to the pulsar surface) [35,36,129,130,136,[142][143][144][145][146][147][148]; 3) Consider other effects/models that can modify the maximum mass of neutron star, such as magnetic field [138], twin star [149], two family compact star [132], finite-temperature [144], antikaon condensation [150], or net electric charge [134], etc.…”
Section: Is Gw190814's Secondary a Superfast And Supermassive Neutron...mentioning
confidence: 99%