2023ApJ...959...97C


Query : 2023ApJ...959...97C

2023ApJ...959...97C - Astrophys. J., 959, 97 (2023/December-3)

Fermi-LAT Detection of the Supernova Remnant G312.4-0.4 in the Vicinity of 4FGL J1409.1-6121e.

CHAMBERY P., LEMOINE-GOUMARD M., JARDIN-BLICQ A., SINHA A. and EAGLE J.

Abstract (from CDS):

Gamma-ray emission provides constraints on the nonthermal radiation processes at play in astrophysical particle accelerators. This allows both the nature of accelerated particles and the maximum energy that they can reach to be determined. Notably, it remains an open question to what extent supernova remnants contribute to the sea of Galactic cosmic rays. In the Galactic plane, at around 312° of Galactic longitude, Fermi-LAT observations show an extended source (4FGL J1409.1-6121e) around five powerful pulsars. This source is described by one large disk of 0.°7 radius with a high significance of 45σ in the 4FGL-DR3 catalog. Using 14 yr of Fermi-LAT observations, we revisited this region with a detailed spectro-morphological analysis in order to disentangle its underlying structure. Three sources have been distinguished, including the supernova remnant G312.4-0.4 whose gamma-ray emission correlates well with the shell observed at radio energies. The hard spectrum detected by the LAT, extending up to 100 GeV without any sign of a cutoff, is well reproduced by a purely hadronic model.

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

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

Simbad objects: 11

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Number of rows : 11
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 NAME Pup A SNR 08 24 07 -42 59.8           ~ 636 1
2 2MASS J14045171-6115578 LP? 14 04 51.7296255222 -61 15 57.878522475           ~ 2 0
3 2MASS J14051441-6118282 HXB 14 05 14.41560 -61 18 28.2168           O6.5III 53 0
4 PSR J1406-6121 Psr 14 06 50.04 -61 21 27.9           ~ 29 0
5 4FGL J1409.1-6121e gam 14 09 10.6 -61 21 11           ~ 6 0
6 PSR J1410-6132 Psr 14 10 24.000 -61 32 00.00           ~ 133 1
7 PSR J1412-6145 Psr 14 12 07.69 -61 45 28.8           ~ 45 1
8 SNR G312.4-00.4 SNR 14 13 00 -61 44.0           ~ 96 1
9 PSR J1413-6141 Psr 14 13 09.87 -61 41 13.0           ~ 44 1
10 PSR J1413-6205 Psr 14 13 30.135 -62 05 37.02           ~ 50 0
11 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1

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