The rp-process in X-ray bursts

Author(s):  
H. Schatz ◽  
L. Bildsten ◽  
J. Görres ◽  
M. Wiescher ◽  
F.-K. Thielemann
Keyword(s):  
X Ray ◽  
2012 ◽  
Vol 21 (08) ◽  
pp. 1250074 ◽  
Author(s):  
CHIRASHREE LAHIRI ◽  
G. GANGOPADHYAY

Densities from relativistic mean field calculations are applied to construct the optical potential and, hence calculate the endpoint of the rapid proton capture (rp) process. Mass values are taken from a new phenomenological mass formula. Endpoints are calculated for different temperature-density profiles of various X-ray bursters. We find that the rp process can produce significant quantities of nuclei upto around mass 95. Our results differ from existing works to some extent.


2017 ◽  
Vol 606 ◽  
pp. A130 ◽  
Author(s):  
J. J. M. in ’t Zand ◽  
M. E. B. Visser ◽  
D. K. Galloway ◽  
J. Chenevez ◽  
L. Keek ◽  
...  

2007 ◽  
Vol 671 (2) ◽  
pp. L141-L144 ◽  
Author(s):  
Alexander Heger ◽  
Andrew Cumming ◽  
Duncan K. Galloway ◽  
Stanford E. Woosley
Keyword(s):  
Type I ◽  
X Ray ◽  

2010 ◽  
Author(s):  
Hendrik Schatz
Keyword(s):  
X Ray ◽  

1996 ◽  
Vol 165 ◽  
pp. 29-41
Author(s):  
Philipp Podsiadlowski

Thorne-Żytkow objects (TŻOs) are red supergiants with neutron cores. The energy source in TŻOs with low-mass envelopes (≲8 M⊙) is accretion onto the neutron core, while for TŻOs with massive envelopes (≲14 M⊙) it is nuclear burning via the exotic rp process. TŻOs are expected to form as a result of unstable mass transfer in high-mass X-ray binaries, the direct collision of a neutron star with a massive companion after a supernova or the collision of a neutron star with a low-mass star in a globular cluster. We estimate a birth rate of massive TŻOs in the Galaxy of ∼2 10−4 yr−1. Thus, for a characteristic TŻO lifetime of 105–106 yr there should be 20–200 TŻOs in the Galaxy at present. These can be distinguished from ordinary red supergiants because of anomalously high surface abundances of lithium and rp-process elements, produced in the TŻO interior. The TŻO phase ends when either the star has exhausted its rp-process seed elements or the envelope mass decreases below a critical mass (∼14 M⊙). Then nuclear burning becomes inefficient and a neutrino runaway ensues, leading to the dynamical accretion of matter near the core onto the neutron star and its spin up to spin frequencies of up to ∼100 Hz. The fate of the massive envelope is not entirely clear. If a significant fraction can be accreted onto the core, the formation of a black hole becomes likely. Part of the envelope may collapse into a massive disk which may ultimately become gravitationally unstable and lead to the formation of planets or even low-mass stars. We discuss the various possible outcomes and suggest a possible link between massive TŻOs and soft X-ray transients.


2010 ◽  
Author(s):  
A. Matthew Amthor ◽  
Daniel Galaviz ◽  
Alexander Heger ◽  
Alexander Sakharuk ◽  
Hendrik Schatz ◽  
...  
Keyword(s):  
Type I ◽  
X Ray ◽  

1999 ◽  
Author(s):  
Michael Wiescher ◽  
Ani Aprahamian ◽  
Joachim Döring ◽  
Joachim Görres
Keyword(s):  
X Ray ◽  

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