scholarly journals Slowly rotating superfluid Newtonian neutron star model with entrainment

2002 ◽  
Vol 381 (1) ◽  
pp. 178-196 ◽  
Author(s):  
R. Prix ◽  
G. L. Comer ◽  
N. Andersson
Keyword(s):  
2009 ◽  
Author(s):  
Valery Suleimanov ◽  
Thomas Rauch ◽  
Klaus Werner ◽  
Alexander Y. Potekhin ◽  
Juri Poutanen ◽  
...  
Keyword(s):  

1992 ◽  
Vol 128 ◽  
pp. 222-224
Author(s):  
Qiao G. J.

AbstractAn induced-collapse model [hereafter IC model; He et al. (1990)] can overcome the problems of the single star model of SN1987A. According to the IC model, there is a possibility that the SN1987A remnant will be a binary system with two neutron stars, one of them (SK-69 202) will have a strong magnetic field and a high surface temperature which favors detection as an X-ray or γ-ray pulsar. If the surface temperature of the neutron star cools down to T = 107 K, a radio binary pulsar is expected. There is also the possibility that an X-ray or γ-ray pulsar will be observed first, and only later will a radio pulsar will be detected.A newly formed neutron star is thought to have a short (millisecond) period. In this case, the core emission beam is then very large (Qiao 1992) and is thus very likely to swing in the direction of the Earth.


1986 ◽  
Vol 221 (2) ◽  
pp. 409-426 ◽  
Author(s):  
A. J. Foster ◽  
R. R. Ross ◽  
A. C. Fabian
Keyword(s):  

1987 ◽  
Vol 125 ◽  
pp. 233-243
Author(s):  
H. Inoue

The maximum peak luminosity of the X-ray bursts from a burster is most likely interpreted as the Eddington luminosity of a helium-rich envelope surrounding a neutron star. If this interpretation is true, we can obtain a relation between the mass and the radius of the neutron star in terms of the maximum effective temperature of bursts. On the other hand, the most naive understanding of the origin of the 4.1 keV absorption line often detected in X-ray burst spectra gives us another relation of the neutron star mass with its radius. By solving two simultaneous equations, we can determine the values of the mass and the radius of the neutron star, respectively. However, the result is critical to every neutron star model currently considered.The persistent emissions from X-ray bursters are also discussed.


1996 ◽  
Vol 165 ◽  
pp. 73-79
Author(s):  
Ene Ergma ◽  
Marek J. Sarna

Possible models for the matter source inside the eclipsing binary system PSR 1718–19, and for the evolution of this system are reviewed, including Zwitter's (1993) stripped main-sequence (MS) turnoff star model. Both the accretion induced collapse (AIC) scenario with a young neutron star, and the capture scenario with an old neutron star are discussed. Although Burderi & King (1994) claim that the size of the Roche lobe (∼0.5 R⊙) unambiguously rules out the AIC formation scenario, we show that in our evolutionary picture an AIC scenario will be possible.


1971 ◽  
Vol 2 ◽  
pp. 731-736
Author(s):  
A. G. W. Cameron

One of the major questions which has been raised with the rotating neutron star model of pulsars, is whether cosmic rays can be produced by the pulsar phenomenon through the acceleration of the surface material of neutron stars. It is therefore very instructive to review the calculations which have been made on the surface structure and cooling histories of neutron stars.Figure 1 shows a diagram of the interior of a neutron star, one of a sequence of models calculated by Cohen et al. (1970). In this diagram the radii of the various parts of the model are to scale. The total radius of the model is 13.7 km. Over a fairly large range of distance downwards from the surface, ions and electrons also put in an appearance, and below that there is a still narrower strip where protons coexist with the ions, electrons, and neutrons. Below this the ions disappear, and at still greater depths mu mesons put in an appearance. Finally, near the center of the star, the calculations indicated that other hyperons probably appear.The region containing the ions can be expected to form a crystalline solid, except in the outer fringes of the atmosphere, where thermal effects and the relatively small pressure will vaporize any crystals.


1990 ◽  
Vol 167 (1) ◽  
pp. 41-53 ◽  
Author(s):  
P. S. Negi ◽  
A. K. Pande ◽  
M. C. Durgapal
Keyword(s):  

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