2021A&A...653A..62C


Query : 2021A&A...653A..62C

2021A&A...653A..62C - Astronomy and Astrophysics, volume 653A62-62 (2021/9-1)

Thermal radio absorption as a tracer of the interaction of SNRs with their environments.

CASTELLETTI G., SUPAN L., PETERS W.M. and KASSIM N.E.

Abstract (from CDS):

We present new images and continuum spectral analysis for 14 resolved Galactic supernova remnants (SNRs) selected from the 74 MHz Very Large Array Low-Frequency Sky Survey Redux (VLSSr). We combine new integrated measurements from the VLSSr with, when available, flux densities extracted from the Galactic and Extragalactic All-Sky Murchison Widefield Array Survey and measurements from the literature to generate improved integrated continuum spectra sampled from ∼15 MHz to ∼217GHz. We present the VLSSr images. When possible we combine them with publicly available images at 1.4GHz, to analyse the resolved morphology and spectral index distribution across each SNR. We interpret the results and look for evidence of thermal absorption caused by ionised gas either proximate to the SNR itself, or along its line of sight. Three of the SNRs, G4.5+6.8 (Kepler), G28.6-0.1, and G120.1+1.4 (Tycho), have integrated spectra which can be adequately fit with simple power laws. The resolved spectral index map for Tycho confirms internal absorption which was previously detected by the Low Frequency Array, but it is insufficient to affect the fit to the integrated spectrum. Two of the SNRs are pulsar wind nebulae, G21.5-0.9 and G130.7+3.1 (3C 58). For those we identify high-frequency spectral breaks at 38 and 12GHz, respectively. For the integrated spectra of the remaining nine SNRs, a low frequency spectral turnover is necessary to adequately fit the data. In all cases we are able to explain the turnover by extrinsic thermal absorption. For G18.8+0.3 (Kes 67), G21.8-0.6 (Kes 69), G29.7-0.3 (Kes 75), and G41.1-0.3 (3C 397), we attribute the absorption to ionised gas along the line of sight, possibly from extended HII region envelopes. For G23.3-0.3 (W41) the absorption can be attributed to HII regions located in its immediate proximity. Thermal absorption from interactions at the ionised interface between SNR forward shocks and the surrounding medium were previously identified as responsible for the low frequency turnover in SNR G31.9+0.0 (3C 391); our integrated spectrum is consistent with the previous results. We present evidence for the same phenomenon in three additional SNRs G27.4+0.0 (Kes 73), G39.2-0.3 (3C 396), and G43.3-0.2 (W49B), and derive constraints on the physical properties of the interaction. This result indicates that interactions between SNRs and their environs should be readily detectable through thermal absorption by future low frequency observations of SNRs with improved sensitivity and resolution.

Abstract Copyright: © ESO 2021

Journal keyword(s): ISM: supernova remnants - radio continuum: general

Simbad objects: 30

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Number of rows : 30
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 SNR G130.7+03.1 SNR 02 05 35.73 +64 49 41.3           ~ 661 4
3 PSR J0205+6449 Psr 02 05 37.92 +64 49 42.8           ~ 268 1
4 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
5 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1314 1
6 AJG 44 Psr 16 17 33.000 -51 02 00.00           ~ 552 3
7 NAME Kepler's SN SNR 17 30 40.51 -21 29 14.4           ~ 851 3
8 NAME Sgr A West HII 17 45 39.4 -29 00 24           ~ 381 0
9 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
10 NAME Sgr A East SNR 17 45 41 -29 00.8           ~ 523 2
11 SNR G006.4-00.1 SNR 18 00 31.2011719 -23 25 48.001099           ~ 782 1
12 SNR G018.8+00.3 SNR 18 24.0 -12 23           ~ 112 0
13 [ABB2014] WISE G021.884-00.318 IR 18 32 12 -09 57.8           ~ 2 0
14 SNR G021.8-00.6 SNR 18 32 45 -10 08.0           ~ 137 0
15 SNR G021.5-00.9 SNR 18 33 33.612 -10 34 07.69           ~ 490 1
16 SNR G023.3-00.3 SNR 18 34 51.80 -08 44 38.2           ~ 240 0
17 SNR G027.3+00.0 SNR 18 41 17.8 -04 56 12           ~ 345 3
18 PSR J1841-0456 Psr 18 41 19.29 -04 56 11.4           ~ 296 1
19 SNR G028.6-00.1 SNR 18 43 55 -03 53.0           ~ 64 1
20 SNR G029.7-00.3 SNR 18 46 22.8 -02 59 47           ~ 375 2
21 PSR J1846-0258 Psr 18 46 24.75 -02 58 29.6           ~ 388 2
22 SNR G031.9+00.0 SNR 18 49 16.3 -00 55 01           ~ 368 2
23 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 1034 2
24 SNR G039.2-00.3 SNR 19 04 03.9 +05 26 56           ~ 204 1
25 [ABB2014] WISE G041.126-00.232 bub 19 07 18.5 +07 10 32           ~ 2 0
26 SNR G041.1-00.3 SNR 19 07 22.6 +07 10 44           ~ 252 2
27 W 49b SNR 19 11 09.5 +09 06 21           ~ 500 1
28 [ABB2014] WISE G043.305-00.211 IR 19 11 17 +09 07.4           ~ 1 0
29 CORNISH G043.3064-00.2114 Y*O 19 11 17.05 +09 07 29.0           ~ 7 0
30 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1

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