Kaon Condensation in the Neutron Star with a Quark-Meson Coupling Model

2011 ◽  
Vol 59 (2(3)) ◽  
pp. 2114-2117
Author(s):  
C. H. Hyun
2011 ◽  
Vol 01 ◽  
pp. 177-182
Author(s):  
C. Y. RYU ◽  
MYUNG-KI CHEOUN

We investigate the structure of neutron star within the framework of the quark-meson coupling model, considering hyperons and kaon condensation. In order to compare the EoS with that from quark matter, the MIT bag model is used. We calculate the mass and radius of a neutron star by using Tolman-Oppenheimer-Volkov equations.


2014 ◽  
Vol 89 (6) ◽  
Author(s):  
D. L. Whittenbury ◽  
J. D. Carroll ◽  
A. W. Thomas ◽  
K. Tsushima ◽  
J. R. Stone

2020 ◽  
Vol 232 ◽  
pp. 03001
Author(s):  
S. Antić ◽  
J. R. Stone ◽  
A. W. Thomas

Recent years continue to be an exciting time for the neutron star physics, providing many new observations and insights to these natural ‘laboratories’ of cold dense matter. To describe them, there are many models on the market but still none that would reproduce all observed and experimental data. The quark-meson coupling model stands out with its natural inclusion of hyperons as dense matter building blocks, and fewer parameters necessary to obtain the nuclear matter equation of state. The latest advances of the QMC model and its application to the neutron star physics will be presented, within which we build the neutron star’s outer crust from finite nuclei up to the neutron drip line. The appearance of different elements and their position in the crust of a neutron star is explored and compared to the predictions of various models, giving the same quality of the results for the QMC model as for the models when the nucleon structure is not taken into account.


2013 ◽  
Vol 54 (7-10) ◽  
pp. 1591-1594 ◽  
Author(s):  
Tsuyoshi Miyatsu ◽  
Koichi Saito

1999 ◽  
Vol 60 (1) ◽  
Author(s):  
S. Pal ◽  
M. Hanauske ◽  
I. Zakout ◽  
H. Stöcker ◽  
W. Greiner

2010 ◽  
Vol 19 (11) ◽  
pp. 2247-2263 ◽  
Author(s):  
ZHONG-MING NIU ◽  
CHUN-YUAN GAO

The properties of neutron stars are investigated by including δ meson field in the modified quark–meson coupling model. It is found that δ meson has opposite effects on hadronic matter with or without hyperons: it softens the EOSs of hadronic matter with hyperons, while it stiffens the EOSs of pure nucleonic matter. Moreover, by replacing the isovector mesons with the contact scalar–isovector interaction, a considerable change of proton fraction is observed. It is shown that the contact scalar–isovector interaction provides an approach to satisfy the constraint of Direct Urca critical star masses. However, the inclusion of δ meson increases the proton fraction, consequently it decreases the M DU which departs farther from the Direct Urca constraint. Furthermore, the inclusion of δ meson field can increase the maximum mass of neutron star and enlarge the corresponding radius, while these quantities are decreased when the contact scalar–isovector interaction is included.


2020 ◽  
Vol 102 (6) ◽  
Author(s):  
S. Antić ◽  
J. R. Stone ◽  
J. C. Miller ◽  
K. L. Martinez ◽  
P. A. M. Guichon ◽  
...  

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