2024RAA....24a5012S


Query : 2024RAA....24a5012S

2024RAA....24a5012S - Research in Astron. and astroph., 24, part no 1, 5012 (2024/January-0)

Point-symmetry in SNR G1.9+0.3: A Supernova that Destroyed its Planetary Nebula Progenitor.

SOKER N.

Abstract (from CDS):

I analyze a new X-ray image of the youngest supernova remnant (SNR) in the Galaxy, which is the type Ia SNR G1.9+0.3, and reveal a very clear point-symmetrical structure. Since explosion models of type Ia supernovae (SNe Ia) do not form such morphologies, the point-symmetrical morphology must come from the circumstellar material (CSM) into which the ejecta expands. The large-scale point-symmetry that I identify and the known substantial deceleration of the ejecta of SNR G1.9+0.3 suggest a relatively massive CSM of ≳1M⊙. I argue that the most likely explanation is the explosion of this SN Ia into a planetary nebula. The scenario that predicts a large fraction of SN Ia inside PNe (SNIPs) is the core degenerate scenario. Other SN Ia scenarios might lead to only a very small fraction of SNIPs or none at all.

Abstract Copyright: © 2023. National Astronomical Observatories

Journal keyword(s): (stars:) supernovae: general - ISM: supernova remnants - (stars:) binaries (including multiple): close - (ISM:) planetary nebulae: general - stars: jets

Simbad objects: 9

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Number of rows : 9
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 SN 1572A SN* 00 25 21.5 +64 08 27           B8 1254 1
2 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
3 M 37 OpC 05 52 18.6 +32 32 36           ~ 436 0
4 IPHASX J055226.2+323724 PN 05 52 26.1908041080 +32 37 24.888501948           PG1159/DO 24 0
5 SN 2018evt SN* 13 46 39.32 -09 38 36.6           SNIa 24 0
6 SS 293 pA* 17 03 10.0705512504 -47 00 27.731886516           Ae 93 0
7 SNR G001.9+00.3 SNR 17 48 46.02 -27 09 52.0           ~ 243 1
8 SNR G041.1-00.3 SNR 19 07 22.6 +07 10 44           ~ 252 2
9 NGC 6826 PN 19 44 48.1500225888 +50 31 30.249034932   9.779 9.359 10.775   O3f(H) 736 0

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