2017
DOI: 10.1103/physrevc.95.065803
|View full text |Cite
|
Sign up to set email alerts
|

Hypernuclei and massive neutron stars

Abstract: Background: The recent accurate measurement of the mass of two pulsars close to or above 2 M has raised the question of whether such large pulsar masses allow for the existence of exotic degrees of freedom, such as hyperons, inside neutron stars. Purpose: In the present work, we will investigate, within a phenomenological relativistic mean field approach, how the existing hypernuclei properties may constrain the neutron star equation of state and confront the neutron star maximum masses obtained with equations… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

6
122
0

Year Published

2017
2017
2023
2023

Publication Types

Select...
7
1

Relationship

1
7

Authors

Journals

citations
Cited by 127 publications
(128 citation statements)
references
References 134 publications
(163 reference statements)
6
122
0
Order By: Relevance
“…(ii) Throughout our work we have focused on a ΛΞ − hyperon composition. For a number of EoS models, Σ − appears in the core (for instance, in deep layers of massive NL3ωρ and FSU2H stars; see also [21][22][23]). The relation between ζ and λ inferred in Sec.…”
Section: Discussionmentioning
confidence: 99%
“…(ii) Throughout our work we have focused on a ΛΞ − hyperon composition. For a number of EoS models, Σ − appears in the core (for instance, in deep layers of massive NL3ωρ and FSU2H stars; see also [21][22][23]). The relation between ζ and λ inferred in Sec.…”
Section: Discussionmentioning
confidence: 99%
“…The relative stability of x sΞ to the modification of the nucleonic EoS, for each considered scenario, reflects the relatively small dispersion among the considered EoS, over the subsaturation density domain explored by a hyperon bound in a nucleus. Note that a similar situation corresponds, according to [8][9][10], also to x sΛ and the explication is the same.…”
Section: B Hyperonic Eos With Calibrated Meson Couplingsmentioning
confidence: 91%
“…Without the coupling to σ * , the Y Y interaction is very repulsive already at low densities. We obtain U ( ) (n sat /5) = 7 MeV, U ( ) (n sat /5) = 47 MeV, and U ( ) (n sat /5) = 26 MeV, whereas the data on double--hypernuclei suggest a weakly attractive potential at least for hyperons, U ( ) (n sat /5) ≈ −1 to −5 MeV [73,75,76]. Although, as shown, e.g., in Refs.…”
Section: B Homogeneous Mattermentioning
confidence: 94%
“…We will assume here standard values [40,70,73] in symmetric nuclear matter at saturation density n sat : U (N) (n sat ) = −30 MeV, U (N) (n sat ) = −18 MeV, and U (N) (n sat ) = +30 MeV. The resulting values are in the range obtained by calculating directly properties of single hypernuclei; see Refs.…”
Section: B Homogeneous Mattermentioning
confidence: 99%
See 1 more Smart Citation