2024A&A...692A.193L


Query : 2024A&A...692A.193L

2024A&A...692A.193L - Astronomy and Astrophysics, volume 692A193 (2024/12-1)

The MeerKAT view on Galactic supernova remnants.

LORU S., INGALLINERA A., UMANA G., BORDIU C., BUEMI C., BUFANO F., CAVALLARO F., LETO P., RIGGI S., TRIGILIO C., THOMPSON M.A., COTTON W.D., GOEDHART S., ANDERSON L.D. and CHIBUEZE J.O.

Abstract (from CDS):

Context. The integrated radio spectrum of supernova remnants (SNRs) and the spatial variation of the spectral indices across these extended sources are powerful tools for studying the shocks and particle acceleration processes occurring in different SNR regions. Characterization of these processes requires sensitive flux density measurements and high-resolution images, which are not always available due to observing difficulties.
Aims. We want to show the potentiality of the high-resolution SARAO MeerKAT legacy Galactic Plane Survey (SMGPS) images regarding the morphological and spectral characterization of 29 known galactic SNRs.
Methods. We used the SMGPS data at 1.284 GHz coupled with data from the GaLactic and Extragalactic All-sky Murchison Widefield Array (GLEAM) survey (0.072-0.231 GHz) to characterize the integrated spectrum of each source and search for spatial spectral variation through analysis of sensitive spectral index maps.
Results. We were able to redefine the exact morphology of four SNRs (G024.7-00.6, G051.4+00.7, G348.7+0.3, and G351.9+00.1), distinguishing them from unrelated sources or identifying new emission regions associated with them and never observed before. In many other cases, we identified in the SMGPS images several H II regions overlaid with the remnants, and we were able to estimate their spectral contribution through inspection of the spatial variation of the spectral indices across the remnants. The integrated spectral indices show a more uniform distribution with respect to what is obtained by considering the values reported in the literature.
Conclusions. We show that new sensitive and high-resolution data are crucial to firmly constraining both the integrated and spatially resolved spectrum of SNRs, especially for the less studied objects of the southern hemisphere. The comparison of our SMGPS-GLEAM spectral index maps with IR, molecular, and γ-ray images allowed us to investigate the nature of the peculiar remnant regions.

Abstract Copyright: © The Authors 2024

Journal keyword(s): radiation mechanisms: non-thermal - ISM: supernova remnants - radio continuum: general

Simbad objects: 59

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Number of rows : 59
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 SNR G166.0+04.3 SNR 05 26 30.000 +42 56 00.00           ~ 196 0
2 W 11 Rad 05 36.2 +23 13           ~ 4 0
3 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1314 1
4 V* V906 Car No* 10 36 15.4286177568 -59 35 53.696262804           ~ 108 1
5 NAME MSH 11-61A SNR 10 59 25.36 -61 18 42.6           ~ 187 0
6 SMSP 6 WR* 11 01 02.0908384608 -60 14 01.029637428 15.52 15.23 14.19     WN4b 18 0
7 SNR G289.7-00.3 SNR 11 01.2 -60 18           ~ 22 0
8 SNR G291.0-00.1 SNR 11 11 54 -60 38.0           ~ 104 0
9 PSR J1119-6127 Psr 11 19 14.30 -61 27 49.5           ~ 439 1
10 SNR G292.2-00.5 SNR 11 19.3 -61 28           ~ 98 1
11 SNR G293.8+00.6 SNR 11 35 00 -60 54.0           ~ 40 0
12 PSR J1135-6055 Psr 11 35 08.428 -60 55 36.50           ~ 34 1
13 SNR G296.7-00.9 SNR 11 54 51.0 -63 08 54           ~ 21 0
14 SNR G296.8-00.3 SNR 11 58 30 -62 35.0           ~ 64 0
15 SNR G301.4-01.0 SNR 12 37.9 -63 49           ~ 20 0
16 SNR G332.4+00.1 SNR 16 15 20 -50 42.0           ~ 93 0
17 HESS J1626-490 gam 16 26 04.0 -49 05 13           ~ 18 0
18 SNR G335.2+00.1 SNR 16 27 45.000 -48 47 00.00           ~ 52 0
19 SNR G337.3+01.0 Rad 16 32 42.1 -46 37 35           ~ 49 1
20 SNR G338.1+00.4 SNR 16 38.0 -46 24           ~ 32 0
21 SNR G348.7+00.3 SNR 17 13 43.0 -38 10 12           ~ 134 2
22 [AAB2008] 1 X 17 14 05.7 -38 10 31           ~ 69 1
23 SNR G348.5+00.1 SNR 17 14 31.780 -38 28 34.50           ~ 233 3
24 SNR G348.5-00.0 Rad 17 15 26 -38 28.0           ~ 39 1
25 SNR G351.7+00.8 SNR 17 21.0 -35 27           ~ 29 0
26 SNR G003.8+00.3 SNR 17 52 55 -25 28.0           ~ 25 0
27 HRDS G018.584+00.344 bub 18 23 34.5 -12 34 50           ~ 10 0
28 HRDS G018.630+00.309 bub 18 23 47.3 -12 33 26           ~ 9 0
29 SNR G018.8+00.3 SNR 18 24.0 -12 23           ~ 112 0
30 SNR G019.1+00.2 SNR 18 24.9 -12 07           ~ 22 0
31 HRDS G022.724-00.010 HII 18 32 42 -09 04.7           ~ 6 0
32 SNR G021.8-00.6 SNR 18 32 45 -10 08.0           ~ 137 0
33 2MASS J18324516-0921545 XB* 18 32 45.162 -09 21 54.55           ~ 37 0
34 SNR G022.7-00.2 SNR 18 33 15 -09 13.0           ~ 87 1
35 HRDS G022.730-00.239 HII 18 33 31.9 -09 10 47           ~ 3 0
36 HRDS G023.389-00.148 HII 18 34 26.2 -08 33 11           ~ 3 0
37 HRDS G023.458-00.179 HII 18 34 40 -08 30.4           ~ 3 0
38 SNR G023.3-00.3 SNR 18 34 51.80 -08 44 38.2           ~ 240 0
39 GAL 023.0-00.4 MoC 18 35 -09.0           ~ 5 0
40 SNR G024.7-00.6 SNR 18 38 43 -07 32.0           ~ 54 1
41 HRDS G032.761-00.151 HII 18 51 39.8 -00 13 15           ~ 3 1
42 SNR G032.8-00.1 SNR 18 51 46.9 -00 03 19           ~ 110 2
43 HESS J1852-000 gam 18 52 +00.0           ~ 15 0
44 SNR G033.2-00.6 gam 18 53 41.1 -00 02 20           ~ 56 1
45 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 1034 2
46 PSR B1855+02.1 Psr 18 57 40.90 +02 10 58.0           ~ 16 0
47 PSR B1855+02 Psr 18 57 43.65400 +02 12 41.0000           ~ 65 0
48 SNR G035.6-00.4 SNR 18 57 55 +02 13.0           ~ 56 1
49 HESS J1858+020 gam 18 58 20.0 +02 05 24           ~ 45 0
50 PSR J1907+0631 Psr 19 07 03.816 +06 31 18.90           ~ 26 0
51 SNR G040.5-00.5 SNR 19 07.2 +06 31           ~ 97 0
52 PSR J1907+06 Psr 19 07 54.751 +06 02 15.79           ~ 147 0
53 ARGO J1907+0627 gam 19 08 12.24 +06 23 30.8           ~ 94 0
54 SNR G045.7-00.4 SNR 19 16 24.000 +11 09 00.00           ~ 60 0
55 SNR G046.8-00.3 SNR 19 18 10 +12 09.0           ~ 75 0
56 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1
57 SNR G051.04+00.07 SNR 19 25 06.3 +16 05 30           ~ 8 0
58 SNR G051.21+00.11 SR? 19 25 17 +16 15.6           ~ 11 0
59 SNR G352.2-00.1 SNR ~ ~           ~ 8 0

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