2021ApJ...908..106L


Query : 2021ApJ...908..106L

2021ApJ...908..106L - Astrophys. J., 908, 106-106 (2021/February-2)

Final compact remnants in core-collapse supernovae from 20 to 40 M: the lower mass gap.

LIU T., WEI Y.-F., XUE L. and SUN M.-Y.

Abstract (from CDS):

A mass paucity of compact objects in the range of ∼2-5 M has been suggested by X-ray binary observations, namely, the "lower mass gap." Gravitational wave detections have unlocked another mass measurement method, and aLIGO/Virgo has observed some candidates in the gap. We revisit the numerical simulations on the core-collapse supernovae (CCSNe) for ∼20-40 M progenitor stars with different initial explosion energies. As a result, the lower explosion energy naturally causes more efficient fallback accretion for low-metallicity progenitors, and then the newborn black holes (BHs) in the center of the CCSNe can escape from the gap, but neutron stars cannot easily collapse into BHs in the gap; nevertheless, the final remnants of the solar-metallicity progenitors stick to the gap. If we consider that only drastic CCSNe can be observed and that those with lower explosion energies are universal, the lower mass gap can be reasonably built. The width and depth of the gap are mainly determined by the typical CCSN initial explosion energy and metallicity. One can expect that the future multimessenger observations of compact objects delineate the shape of the gap, which might constrain the properties of the CCSNe and their progenitors.

Abstract Copyright: © 2021. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Accretion - Neutron stars - Core-collapse supernovae - Stellar mass black holes

Errata: erratum vol. 915, art. 72 (2021)

Simbad objects: 7

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Number of rows : 7
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 PSR J0348+0432 Psr 03 48 43.6363173480 +04 32 11.461921260           ~ 267 2
2 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 277 0
3 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2008 0
4 PSR J1614-2230 Psr 16 14 36.5070 -22 30 31.207           ~ 395 1
5 PSR J2215+51 Psr 22 15 32.6869149432 +51 35 36.400854912           ~ 141 0
6 GRB 190425 GWE ~ ~           ~ 318 0
7 GrW 190814 GWE ~ ~           ~ 326 0

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