2011ApJ...732..114L


Query : 2011ApJ...732..114L

2011ApJ...732..114L - Astrophys. J., 732, 114 (2011/May-2)

Using the X-ray morphology of young supernova remnants to constrain explosion type, ejecta distribution, and chemical mixing.

LOPEZ L.A., RAMIREZ-RUIZ E., HUPPENKOTHEN D., BADENES C. and POOLEY D.A.

Abstract (from CDS):

Supernova remnants (SNRs) are a complex class of sources, and their heterogeneous nature has hindered the characterization of their general observational properties. To overcome this challenge, in this paper, we use statistical tools to analyze the Chandra X-ray images of Galactic and Large Magellanic Cloud SNRs. We apply two techniques, a power-ratio method (a multipole expansion) and wavelet-transform analysis, to measure the global and local morphological properties of the X-ray line and thermal emission in 24 SNRs. We find that Type Ia SNRs have statistically more spherical and mirror-symmetric thermal X-ray emission than core-collapse (CC) SNRs. The ability to type SNRs based on thermal emission morphology alone enables, for the first time, the typing of SNRs with weak X-ray lines and those with low-resolution spectra. Based on our analyses, we identify one source (SNR G344.7-0.1) as originating from a CC explosion that was of unknown origin previously; we also confirm the tentative Type Ia classifications of G337.2-0.7 and G272.2-3.2. Although the global morphology is indicative of the explosion type, the relative morphology of the X-ray line emission within SNRs is not: all sources in our sample have well-mixed ejecta, irrespective of stellar origin. In particular, we find that 90% of the bright metal-line-emitting substructures are spatially coincident and have similar scales, even if the metals arise from different burning processes. Moreover, the overall X-ray line morphologies within each SNR are the same, with <6% differences. These findings reinforce observationally that hydrodynamical instabilities can efficiently mix ejecta in Type Ia and CC SNRs. The only exception is W49B, which can be attributed to its jet-driven/bipolar explosive origin. Based on comparative analyses across our sample, we describe several observational constraints that can be used to test hydrodynamical models of SNR evolution; notably, the filling factor of X-ray emission decreases with SNR age.

Abstract Copyright:

Journal keyword(s): ISM: supernova remnants - methods: data analysis - techniques: image processing - X-rays: ISM

Simbad objects: 32

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Number of rows : 32
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 SN 1572A SN* 00 25 21.5 +64 08 27           B8 1188 1
2 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 5838 1
3 SNR G130.7+03.1 SNR 02 05 37.0 +64 49 42           ~ 620 4
4 SNR B0453-68.5 SNR 04 53 36.00 -68 29 30.0           ~ 79 1
5 SNR B0505-67.9 SNR 05 05 42.0 -67 52 29           ~ 141 0
6 SNR J050555-680150 SNR 05 05 55.00 -68 01 54.0           ~ 84 0
7 LHA 120-N 103B EmO 05 08 47.8 -68 45 39           ~ 223 1
8 SNR B0509-67.5 SNR 05 09 31 -67 31.3           ~ 224 0
9 SNR B0519-69.0 SNR 05 19 35.14 -69 02 00.5           ~ 156 0
10 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17434 0
11 SNR J052501-693842 SNR 05 25 02.3 -69 38 39           ~ 401 1
12 SNR B0525-66.0 SNR 05 25 27.1 -65 59 11           ~ 102 1
13 LHA 120-N 206A HII 05 31 15.2 -71 03 58           ~ 108 2
14 SNR J053400-695508 SNR 05 33 59.00 -69 55 00.0           ~ 64 0
15 SNR B0535-66.0 SNR 05 35 43.1 -66 01 59           ~ 175 1
16 SNR B0548-70.4 SNR 05 47 50.00 -70 24 54.0           ~ 87 0
17 SNR G272.2-03.2 SNR 09 06 50 -52 07.0           SNIa 72 0
18 SNR G292.0+01.8 SNR 11 24 59 -59 19.1           ~ 327 1
19 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1328 1
20 AJG 44 Psr 16 17 33.000 -51 02 00.00           ~ 512 3
21 SNR G337.2-00.7 Rad 16 39 15.0 -47 48 27           ~ 62 1
22 SNR G344.7-00.1 SNR 17 03 49 -41 42.5           ~ 87 0
23 QSO B1714-373 BL? 17 18 10.160 -37 18 53.80           ~ 187 0
24 NAME Kepler SNR Rad 17 30 40.5 -21 29 14           ~ 795 4
25 SNR G001.9+00.3 SNR 17 48 46.0 -27 09 52           ~ 209 1
26 SNR G011.2-00.3 SNR 18 11 28.9 -19 25 29           ~ 286 1
27 SNR G015.9+00.2 SNR 18 18 52 -15 02.0           ~ 99 0
28 4C -04.71 Rad 18 41 19.8 -04 56 06           ~ 327 3
29 SNR G033.6+00.1 SNR 18 52 29.000 +00 38 42.00           ~ 285 1
30 W 49b SNR 19 11 09.000 +09 06 24.00           ~ 463 1
31 3C 461 BL? 23 23 24.000 +58 48 54.00     14.30     ~ 2792 1
32 NAME Local Group GrG ~ ~           ~ 8391 0

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