The Impacts of Neutron Star Structure and Base Heating on Type I X-Ray Bursts and Code Comparison

Abstract Type I X-ray bursts are rapidly brightening phenomena triggered by thermonuclear burning on the accreting layers of a neutron star (NS). The light curves represent the physical properties of NSs and the nuclear reactions on the proton-rich nuclei. The numerical treatments of the accreting N...

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Bibliographic Details
Published inThe Astrophysical journal Vol. 950; no. 2; pp. 110 - 120
Main Authors Zhen, Guoqing, Lü, Guoliang, Liu, Helei, Dohi, Akira, Nishimura, Nobuya, Zhu, Chunhua, Song, Liyu, Wang, Weiyang, Xu, Renxin
Format Journal Article
LanguageEnglish
Published The American Astronomical Society 01.06.2023
IOP Publishing
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Summary:Abstract Type I X-ray bursts are rapidly brightening phenomena triggered by thermonuclear burning on the accreting layers of a neutron star (NS). The light curves represent the physical properties of NSs and the nuclear reactions on the proton-rich nuclei. The numerical treatments of the accreting NS and physics of the NS interior are not established, which shows uncertainty in modeling for observed X-ray light curves. In this study, we investigate theoretical X-ray burst models compared with burst light curves with GS 1826-24 observations. We focus on the impacts of the NS mass and radius and base heating on the NS surface using the MESA code. We find a monotonic correlation between the NS mass and the parameters of the light curve. The higher the mass, the longer the recurrence time and the greater the peak luminosity. While the larger the radius, the longer the recurrence time, the peak luminosity remains nearly constant. In the case of increasing base heating, both the recurrence time and peak luminosity decrease. We also examine the above results with a different numerical code, HERES , based on general relativity and consider the central NS. We find that the burst rate, energy, and strength are almost the same in two X-ray burst codes by adjusting the base heat parameter in MESA (the relative errors ≲5%), while the duration and rise times are significantly different between (the relative error is possibly ∼50%). The peak luminosity and the e-folding time change irregularly between two codes for different accretion rates.
Bibliography:AAS44576
High-Energy Phenomena and Fundamental Physics
ISSN:0004-637X
1538-4357
DOI:10.3847/1538-4357/accd5f