2022ApJ...940L..27W


Query : 2022ApJ...940L..27W

2022ApJ...940L..27W - Astrophys. J., 940, L27 (2022/November-3)

Extreme Mass Loss in Low-mass Type Ib/c Supernova Progenitors.

WU S.C. and FULLER J.

Abstract (from CDS):

Many core-collapse supernovae (SNe) with hydrogen-poor and low-mass ejecta, such as ultra-stripped SNe and type Ibn SNe, are observed to interact with dense circumstellar material (CSM). These events likely arise from the core collapse of helium stars that have been heavily stripped by a binary companion and have ejected significant mass during the last weeks to years of their lives. In helium star models run to days before core collapse we identify a range of helium core masses ≈2.5-3 M⊙ whose envelopes expand substantially due to the helium shell burning while the core undergoes neon and oxygen burning. When modeled in binary systems, the rapid expansion of these helium stars induces extremely high rates of late-stage mass transfer ($\dot{M}\gtrsim {10}^{-2}\,{M}_{\odot }\,{\mathrm{yr}}^{-1}$) beginning weeks to decades before core collapse. We consider two scenarios for producing CSM in these systems: either mass transfer remains stable and mass loss is driven from the system in the vicinity of the accreting companion, or mass transfer becomes unstable and causes a common envelope event (CEE) through which the helium envelope is unbound. The ensuing CSM properties are consistent with the CSM masses (∼10–2-1 M⊙) and radii (∼1013-1016 cm) inferred for ultra-stripped SNe and several type Ibn SNe. Furthermore, systems that undergo a CEE could produce short-period neutron star binaries that merge in less than 100 Myr.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Core-collapse supernovae - Binary stars - Stellar mass loss - Circumstellar matter - Stellar evolution

Simbad objects: 11

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Number of rows : 11
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 LSQ 13ddu SN* 03 58 49.09 -29 25 11.8           SNIa 15 0
2 SN 2006jc SN* 09 17 20.78 +41 54 32.7     13.8     SNIbn 380 1
3 SN 2019wep SN* 11 04 37.033 +45 58 38.95           SNII-pec 13 0
4 SN 2019uo SN* 12 02 36.602 +41 03 41.92           SNIbn 27 0
5 iPTF 15ul SN* 12 14 03.76 +47 54 03.9           ~ 24 0
6 SN 2019deh SN* 14 05 43.577 +09 30 56.77           SNIbn 11 0
7 SN 2021jpk SN* 14 39 00.025 +12 40 10.02           SNIbn 5 0
8 SN 2019hgp SN* 15 36 12.90 +39 44 00.6           SNIcn 29 0
9 SN 2019dge SN* 17 36 46.742 +50 32 52.12           SNIb 32 0
10 SN 2019jc SN* 21 55 40.99 +24 54 20.6           SNIcn 12 0
11 SN 2014ft SN* 23 33 27.95 +33 38 46.1           SNIc 58 0

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