2018ApJ...859...69A


Query : 2018ApJ...859...69A

2018ApJ...859...69A - Astrophys. J., 859, 69-69 (2018/May-3)

GeV emission in the region of HESS J1809-193 and HESS J1813-178 is HESS J1809-193 a proton pevatron?

ARAYA M.

Abstract (from CDS):

HESS J1809-193 is an unidentified TeV source discovered by the High Energy Stereoscopic System and originally classified as a pulsar wind nebula (PWN) candidate associated with the pulsar PSR J1809-1917. However, a recent study of deep radio observations and the interstellar medium near the source has found evidence for a hadronic scenario for the gamma-rays. Here, a detailed study of the GeV emission in the region using data from the Fermi-LAT is presented. The GeV emission has an extended morphology in the region of the TeV emission and the overall spectrum can be accounted for by a cosmic-ray population having a simple power-law spectrum with energies extending up to 1 PeV. However, the spectrum at tens of TeV should be observed more deeply in the future to confirm its hadronic nature, and other scenarios involving combinations of leptonic and hadronic emission from several of the known supernova remnants in the region cannot be ruled out. The nearby TeV source HESS J1813-178, thought to be a PWN, is also studied in detail at GeV energies and we find a region of significant emission that is much more extended than the TeV emission and whose spectrum is softer than expected from a PWN but similar to those seen in several star-forming regions that are believed to accelerate protons. There is marginal evidence for a GeV point source at the location of the X-ray PWN, beside the extended emission.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): gamma rays: ISM - ISM: individual: (object HESS J809-193,HESS J1813-178) - ISM: supernova remnants

Simbad objects: 34

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Number of rows : 34
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1237 1
2 NAME Vela X Psr 08 33 08.880 -45 11 24.36           ~ 282 1
3 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 14436 0
4 SNR G006.4-00.1 SNR 18 00 31.2011719 -23 25 48.001099           ~ 738 1
5 PSR B1757-24 Psr 18 01 00.016 -24 51 27.50           ~ 244 1
6 1AGLR J1807-2103 gam 18 03 52.1 -21 10 54           ~ 73 0
7 4FGL J1804.7-2144e BL? 18 04 45.8 -21 44 06           ~ 6 0
8 W 30 BL? 18 05 31.2011719 -21 25 48.001099           ~ 174 1
9 Fermi J1808.2-2029 gam 18 08 00.0 -20 24 00           ~ 16 0
10 [HJK2000] GC01 GlC 18 08 21.8 -19 49 47           ~ 58 0
11 SNR G007.5-01.7 SNR 18 09 -23.3           ~ 11 0
12 PSR B1806-19.3 Psr 18 09 43.147 -19 17 38.10           ~ 101 1
13 SNR G011.1+00.1 SNR 18 09.8 -19 12           ~ 26 0
14 SNR G011.0+00.0 SNR 18 10.1 -19 25           ~ 35 1
15 3FGL J1810.1-1910 BL? 18 10 11 -19 10.1           ~ 8 0
16 XTE J1810-189 LXB 18 10 20.86 -19 04 11.2           ~ 56 0
17 HESS J1809-193 gam 18 10 31 -19 18.0           ~ 54 1
18 SNR G011.4-00.1 SNR 18 10.8 -19 05           ~ 55 0
19 Suzaku J1811-1900 XB? 18 11.0 -19 00           ~ 3 0
20 SNR G011.2-00.3 SNR 18 11 28.9 -19 25 29           ~ 286 1
21 PSR J1811-1926 Psr 18 11 29.15 -19 25 25.4           ~ 126 1
22 3FHL J1811.5-1927 gam 18 11 32.432 -19 27 03.30           ~ 2 0
23 3FGL J1811.3-1927c BL? 18 11 32.8 -19 25 39           ~ 10 0
24 2FGL J1811.3-2421 gam 18 11 32.80 -24 22 47.8           ~ 9 0
25 SNR G012.5+00.2 Rad 18 12.2 -17 55           ~ 17 1
26 SNR G012.7+00.0 SNR 18 13.3 -17 54           ~ 22 0
27 NAME AGPS 273.4-17.8 SNR 18 13 35.05 -17 49 58.1           ~ 125 2
28 SNR G012.8-00.0 SNR 18 13.6 -17 49           ~ 62 0
29 3FGL J1814.0-1757c gam 18 14 03 -17 57.7           ~ 6 0
30 1AGL J1815-1732 gam 18 14 05 -17 36.1           ~ 27 0
31 SNR G013.5+00.2 SNR 18 14.2 -17 12           ~ 25 0
32 SNR G012.8-00.2 SFR 18 14 14.0 -17 55 50           ~ 258 0
33 PSR B1823-13 Psr 18 26 13.06 -13 34 48.1           ~ 421 1
34 NAME Cyg X BL? 20 30 04.7973633 +40 51 36.002197           ~ 848 1

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