2012A&A...543A.157B


Query : 2012A&A...543A.157B

2012A&A...543A.157B - Astronomy and Astrophysics, volume 543A, 157-157 (2012/7-1)

Hyperons in neutron-star cores and a 2M pulsar.

BEDNAREK I., HAENSEL P., ZDUNIK J.L., BEJGER M. and MANKA R.

Abstract (from CDS):

A recent measurement of the mass of PSR J1614-2230 rules out most existing models of the equation of state (EOS) of dense matter that is subjected to the high-density softening caused by either hyperonization or a phase transition to either quark matter or a boson condensate. We attempt to resolve the apparent differences between the predictions derived from up-to-date hypernuclear data, which include the appearance of hyperons at about three nuclear densities and the existence of a M=2.0M neutron star. We consider a non-linear relativistic mean field (RMF) model involving the baryon octet coupled to meson fields. An effective Lagrangian includes quartic terms in the meson fields. The values of the model parameters are obtained by fitting the semi-empirical parameters of nuclear matter at the saturation point, as well as potential wells for hyperons in nuclear matter and the strength of the Λ-Λ attraction in double-Λ hypernuclei. We propose a non-linear RMF model that is consistent with up-to-date semi-empirical nuclear and hypernuclear data and allows for neutron stars with hyperon cores and M>2M. The model involves hidden-strangeness scalar and vector mesons, coupled only to hyperons, and quartic terms involving vector meson fields. Our EOS involving hyperons is stiffer than the corresponding nucleonic EOS (in which hyperons are artificially suppressed) above five nuclear densities. The required stiffening is generated by the quartic terms involving the hidden-strangeness vector meson.

Abstract Copyright:

Journal keyword(s): dense matter - equation of state - stars: neutron

Simbad objects: 2

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Number of rows : 2
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 PSR J1614-2230 Psr 16 14 36.5070 -22 30 31.207           ~ 391 1
2 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 158 1

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