2022A&A...659A..97F


Query : 2022A&A...659A..97F

2022A&A...659A..97F - Astronomy and Astrophysics, volume 659A, 97-97 (2022/3-1)

Relativistic Coulomb screening in pulsational pair instability supernovae.

FAMIANO M.A., MORI K., BALANTEKIN A.B., KAJINO T., KUSAKABE M. and MATHEWS G.

Abstract (from CDS):

Context. Pulsational pair-instability supernovae (PPISNe) and pair instability supernovae (PISNe) are the result of a thermonuclear runaway in the presence of a background electron-positron pair plasma. As such, their evolution and resultant black hole masses could possibly be affected by screening corrections due to the electron pair plasma. Aims. The sensitivity of PISNe and PPISNe to relativistic weak screening has been explored. Methods. In this paper a weak screening model that includes effects from relativistic pair production has been developed and applied at temperatures approaching and exceeding the threshold for pair production. This screening model replaces "classical" screening commonly used in astrophysics. Modifications to the weak screening electron Debye length were incorporated in a computationally tractable analytic form. Results. In PPISNe the BH masses were found to increase somewhat at high temperatures, though this increase is small. The BH collapse is also found to occur at earlier times, and the pulsational morphology also changes. In addition to the resultant BH mass, the sensitivity to the screening model of the pulsational period, the pulse structure, the PPISN-to-PISN transition, and the shift in the BH mass gap has been analyzed. The dependence of the composition of the ejected mass was also examined.

Abstract Copyright: © ESO 2022

Journal keyword(s): instabilities - nuclear reactions, nucleosynthesis, abundances - plasmas - relativistic processes - stars: massive

Simbad objects: 3

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Number of rows : 3
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 GrW 170608 GWE ~ ~           ~ 111 0
2 GrW 190521 GWE ~ ~           ~ 285 0
3 GrW 170729 GWE ~ ~           ~ 114 0

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