2024A&A...689A.281M


Query : 2024A&A...689A.281M

2024A&A...689A.281M - Astronomy and Astrophysics, volume 689A281 (2024/9-1)

A look at the high energy aspects of the supernova remnant G309.8+00.0 with eROSITA and Fermi-LAT.

MICHAILIDIS M., PUHLHOFER G., SANTANGELO A., SASAKI M. and BECKER W.

Abstract (from CDS):

Supernova remnant (SNR) detection along the Galactic plane poses a number of challenges. A diffuse X-ray emission component emanating from unidentified sources on the Galactic plane further complicates such a detection in X-rays. Due to the presence of dense dust clouds along the Galactic plane, X-ray photons are also subject to high absorption. Similarly, diffuse signals from the Galactic plane cause γ-ray contamination from the signal of individual objects. The SNR G309.8+00.0 lies exactly on the Galactic plane, with its center coinciding with galactic latitude (b) = 0°. In this paper we report the first detection of the SNR G309.8+00.0 in X-rays and γ rays, using stacked data from the first four consecutive extended ROentgen Survey Imaging Telescope Array (eROSITA) - on board the Russian-German Spektrum Roentgen Gamma (SRG) - all-sky surveys (eRASS:4) and ∼15.5 yr of Pass 8 data recorded from Fermi-LAT, respectively. The SNR appears to have an elliptical shape of 0ọ43 × 0ọ32 in size in both radio synchrotron and X-ray data. The SNR's emission exhibits a shell-like morphology and good spatial correlation in both energy bands. The X-ray emission was solely detected in the 1-2 keV energy band (subject to strong absorption at soft X-rays) and the spectral analysis results of eRASS:4 data present a purely thermal SNR with a high absorption column density 3.1+0.7–0.5 ⋅ 1022 cm–2 and a temperature of 0.34 ± 0.1 keV. Although the thermal plasma appears to be in equilibrium, the limited statistics do not allow us to exclude nonequilibrium models. The X-ray spectral analysis of the remnant resulted in the detection of relatively (given the limited statistics) prominent Mg triplet lines at 1.33-1.47 keV and silicon (Si XIII) at 1.74-1.9 keV energies. In combination with optical extinction data, the absorption column density values derived from the remnant's spectral analysis support a remnant's distance greater than 6 kpc, rather than a 3.12 kpc distance as reported in the literature, and yield an age of 1 - 3.5 ⋅ 105 yr. Employing ∼15.5 yr of Fermi-LAT γ-ray data at and around the remnant's vicinity, we confirm the detection of the to-date unidentified 4FGL J1349.5-6206c source that can either be modeled as a single source or a conglomerate of multiple distinct source components. In the latter case, the detailed inspection of the Fermi-LAT γ-ray data in the direction of the remnant allowed us to decompose the 4FGL J1349.5-6206c source into four point-like components, among which one is spatially coincident with the SNR G309.8+00.0 shell. We detected the component that spatially coincides with the SNR with a significance of 5.8σ above 1 GeV with Fermi-LAT and thus argue that the SNR G309.8+00.0 likely represents at least a significant portion (if not all) of the emission from the 4FGL J1349.5-6206c γ-ray source, detected with 9.8σ significance > 1 GeV with Fermi-LAT.

Abstract Copyright: © The Authors 2024

Journal keyword(s): ISM: supernova remnants - gamma rays: ISM - X-rays: ISM - X-rays: individuals: G309.8+00.0 - acceleration of particles - cosmic rays

Simbad objects: 27

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Number of rows : 27
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 G180.0-01.7 SNR 05 39 00.000 +27 50 00.00           ~ 294 2
2 SNR G279.0+01.1 SNR 09 57.7 -53 15           ~ 37 0
3 PSR J1337-6306 Psr 13 37 20.35 -63 06 23.3           ~ 4 0
4 PSR B1334-61 Psr 13 38 09.24700 -62 04 18.7000           ~ 36 0
5 PSR B1338-62 Psr 13 41 42.63 -62 20 20.7           ~ 152 1
6 PSR J1344-6059 Psr 13 44 39.6 -60 59 31           ~ 3 0
7 PSR J1345-6115 Psr 13 45 44.43 -61 15 30.6           ~ 15 0
8 SNR G309.4-00.1 SNR 13 47 -62.3           ~ 1 0
9 PSR J1348-6307 Psr 13 48 42.4 -63 07 04           ~ 7 0
10 PSR J1349-63 Psr 13 49.3 -63 56           ~ 4 0
11 4FGL J1349.5-6206c gam 13 49 35.2 -62 06 30           ~ 2 0
12 PSR J1349-6130 Psr 13 49 36.65 -61 30 17.1           ~ 33 0
13 PSR J1350-6225 Psr 13 49 43.33 -62 24 02.6           ~ 20 0
14 SNR G309.8+00.0 SNR 13 50 30.000 -62 05 00.00           ~ 48 0
15 2MASS J13503303-6159245 LP? 13 50 33.0486374833 -61 59 24.710233257           ~ 2 0
16 PSR J1354-6249 Psr 13 54 35.0 -62 49 30           ~ 4 0
17 PSR J1355-6206 Psr 13 55 21.3011056920 -62 06 19.419702480           ~ 14 0
18 PSR B1354-62 Psr 13 57 25.0 -62 28 00           ~ 42 0
19 PSR J1358-6025 Psr 13 58 25.8837891 -60 25 55.458069           ~ 21 0
20 PSR B1356-60 Psr 13 59 58.2480 -60 38 07.550           ~ 131 0
21 SNR G310.6-01.6 SNR 14 00 45.69 -63 25 42.6           ~ 45 1
22 PSR J1403-6310 Psr 14 03 14.0 -63 10 27           ~ 9 0
23 SNR G321.3-03.9 SNR 15 32 14.0 -60 51 54           ~ 10 0
24 PSR J1615-5137 Psr 16 15 12.62 -51 34 53.3           ~ 67 0
25 NAME LHB X 16 42.0 +02 19           ~ 414 0
26 NAME Kepler's SN SNR 17 30 40.51 -21 29 14.4           ~ 851 3
27 NAME Cyg Loop SNR 20 51.0 +30 40           ~ 964 0

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