2022ApJ...930...92F


Query : 2022ApJ...930...92F

2022ApJ...930...92F - Astrophys. J., 930, 92-92 (2022/May-1)

The Double Detonation of a Double-degenerate System, from Type Ia Supernova Explosion to its Supernova Remnant.

FERRAND G., TANIKAWA A., WARREN D.C., NAGATAKI S., SAFI-HARB S. and DECOURCHELLE A.

Abstract (from CDS):

Type Ia supernovae (SNe) are believed to be caused by the thermonuclear explosion of a white dwarf (WD), but the nature of the progenitor system(s) is still unclear. Recent theoretical and observational developments have led to renewed interest in double-degenerate models, in particular the "helium-ignited violent merger" or "dynamically driven double-degenerate double-detonation" (D6). In this paper we take the output of an existing D6 SN model and carry it into the supernova remnant (SNR) phase up to 4000 yr after the explosion, past the time when all the ejecta have been shocked. Assuming a uniform ambient medium, we reveal specific signatures of the explosion mechanism and spatial variations intrinsic to the ejecta. The first detonation produces an ejecta tail visible at early times, while the second detonation leaves a central density peak in the ejecta that is visible at late times. The SNR shell is off-center at all times, because of an initial velocity shift due to binary motion. The companion WD produces a large conical shadow in the ejecta, visible in projection as a dark patch surrounded by a bright ring. This is a clear and long-lasting feature that is localized, and its impact on the observed morphology is dependent on the viewing angle of the SNR. These results offer a new way to diagnose the explosion mechanism and progenitor system using observations of a Type Ia SNR.

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

Journal keyword(s): Supernovae - Supernova remnants - Hydrodynamical simulations

Simbad objects: 17

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Number of rows : 17
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 SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
3 SN 2010lp SN* 02 54 03.50 +02 57 43.4           SNIapec 44 1
4 LHA 120-N 103B EmO 05 08 47.8 -68 45 39           ~ 244 1
5 SNR J050854-684447 SNR 05 08 59.26 -68 43 33.9           ~ 157 2
6 SNR B0509-67.5 SNR 05 09 31 -67 31.3           ~ 248 0
7 SNR B0519-69.0 SNR 05 19 35.14 -69 02 00.5           ~ 172 0
8 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
9 SN 2011km SN* 08 09 12.87 +46 18 48.8           SNIa 155 0
10 SN 2014J SN* 09 55 42.12 +69 40 25.9           SNIa-norm 456 1
11 SN 2012cg SN* 12 27 12.83 +09 25 13.2           SNIa-norm 224 1
12 ASASSN -14bd SN* 12 52 44.8 +26 28 13           SNIa 102 0
13 SN 2011fe SN* 14 03 05.711 +54 16 25.22   10.12 10.06     SNIa-norm 747 1
14 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1407 1
15 NAME Kepler's SN SNR 17 30 40.51 -21 29 14.4           ~ 851 3
16 SNR G001.9+00.3 SNR 17 48 46.02 -27 09 52.0           ~ 243 1
17 SNR G070.0-21.5 SNR 21 24.0 +19 23           ~ 28 0

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