2023ApJ...952..158Z


Query : 2023ApJ...952..158Z

2023ApJ...952..158Z - Astrophys. J., 952, 158 (2023/August-1)

4FGL J1844.4-0306: High-energy Emission Likely from the Supernova Remnant G29.37 + 0.1.

ZHENG D., WANG Z., ZHANG X., CHEN Y. and XING Y.

Abstract (from CDS):

Very-high-energy (VHE) observations have revealed approximately 100 TeV sources in our Galaxy, and a significant fraction of them are under investigation to understand their origin. We report our study of one of them, HESS J1844-030. It is found to be possibly associated with the supernova remnant (SNR) candidate G29.37 + 0.1, and detailed studies of the source region at radio and X-ray frequencies have suggested that this SNR is a composite one, containing a pulsar wind nebula (PWN) powered by a candidate young pulsar. As the GeV source 4FGL J1844.4-0306 is also located in the region with high positional coincidence, we analyze its γ-ray data obtained with the Large Area Telescope on board the Fermi Gamma-ray Space Telescope. We determine the GeV γ-ray emission is extended, described with a log-parabola function. The obtained spectrum can be connected to that of the VHE source HESS J1844-030. Given these properties and those from multifrequency studies, we discuss the origin of the γ-ray emission by considering that the two γ-ray sources are associated. Our modeling indicates that while the TeV part would have either a hadronic (from the SNR) or a leptonic origin (from the putative PWN), the GeV part would arise from a hadronic process. Thus we conclude that 4FGL J1844.4-0306 is likely the GeV counterpart to G29.37 + 0.1.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Supernova remnants - Pulsar wind nebulae - Gamma-ray sources

Simbad objects: 14

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Number of rows : 14
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 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
2 3EG J1837-0423 Rad 18 38 52.0 -04 16 16           ~ 95 1
3 SNR G028.8+01.5 SNR 18 39 00.000 -03 00 00.00           ~ 36 1
4 4FGL J1842.2-0328 gam 18 42 14.0 -03 28 57           ~ 6 0
5 1FGL J1842.9-0359c gam 18 42 52.56 -04 00 13.3           ~ 15 0
6 3FGL J1843.7-0322 gam 18 43 43.5 -03 26 13           ~ 12 0
7 1FGL J1844.3-0309c gam 18 44 29 -03 07.0           ~ 12 0
8 PSR J1844-0346 Psr 18 44 32.90 -03 46 26.6           ~ 45 0
9 SNR G029.37+00.1 SNR 18 44 34.3 -03 07 37           ~ 9 0
10 HESS J1844-030 gam 18 44 40.0 -03 06 00           ~ 17 0
11 3XMM J184442.9-030525 X 18 44 42.96 -03 05 25.7           ~ 3 0
12 4FGL J1845.8-0236c gam 18 45 50.1 -02 36 25           ~ 3 0
13 1FGL J1846.8-0233c gam 18 46 55.2 -02 27 08           ~ 18 1
14 4FGL J1847.2-0200c ? 18 47 17.8 -02 00 59           ~ 6 0

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