2022A&A...659A..83S


Query : 2022A&A...659A..83S

2022A&A...659A..83S - Astronomy and Astrophysics, volume 659A, 83-83 (2022/3-1)

Diffuse GeV emission in the field of HESS J1912+101 revisited.

SUN X.-N., YANG R.-Z. and LIANG E.-W.

Abstract (from CDS):

We have analyzed 12 years of Fermi Large Area Telescope data toward the HESS J1912+101 region. With the latest source catalog and diffuse background models, a γ-ray excess is detected with a significance of ∼8σ in the energy range of above 10 GeV. It has been argued that the diffuse GeV emission in the vicinity of HESS J1912+101 are from an extended pulsar wind nebula powered by PSR J1913+1011 and also that the hard GeV emission above 10 GeV stems from the shell-type supernova remnant and is connected with the TeV emissions. Different from previous works, our analysis indicates that the H2 spatial template is preferred over the other spatial templates, suggesting that the diffuse emission component spatially correlates with the dense molecular gas. This spatial correlation favors a hadronic emission scenario, although a leptonic origin cannot be ruled out. In the hadronic scenario, the parent proton spectrum can be described by a power-law function with an index of α = 2.36 ± 0.16. Above 50 GeV, there is no emission, and the upper limits reveal a spectral cutoff or break in the parent proton spectrum that can be explained as propagation effects of cosmic rays. We argue that the parent protons may come from the candidate supernova remnant HESS J1912+101 or the young massive star cluster Mc20.

Abstract Copyright: © ESO 2022

Journal keyword(s): gamma rays: general - galaxies: star clusters: general - ISM: supernova remnants

Simbad objects: 18

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Number of rows : 18
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 NGC 3603 OpC 11 15 10.8 -61 15 32           ~ 1046 1
2 AMS 2 QSO 17 13 15.9 +60 02 34           ~ 16 0
3 SNR G353.6-00.7 SNR 17 31 55.0 -34 42 36           ~ 134 0
4 LBN 028.77+03.43 HII 18 31 26.5 -02 04 22           ~ 227 2
5 RSGC 1 OpC 18 37 58 -06 53.0           ~ 104 0
6 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 950 2
7 4FGL J1908.6+0915e gam 19 08 38.4 +09 15 36           ~ 4 0
8 W 49b SNR 19 11 09.000 +09 06 24.00           ~ 452 1
9 4FGL J1911.7+1014 gam 19 11 43.8 +10 14 25           ~ 4 0
10 [ABB2014] WISE G044.224+00.085 bub 19 11 57.7 +10 07 05           ~ 22 0
11 ARGO J1912+1026 gam 19 12 14.9 +10 21 06           ~ 42 0
12 [MCM2005b] 20 OpC 19 12 25 +09 57.7           ~ 15 0
13 2HWC J1912+099 gam 19 12.4 +09 56           ~ 5 0
14 4FGL J1912.7+0957 gam 19 12 44.4 +09 57 15           ~ 4 0
15 PSR J1913+1011 Psr 19 13 20.341 +10 11 22.97           ~ 69 0
16 4FGL J1914.5+1107 gam 19 14 32.6 +11 07 23           ~ 3 0
17 4FGL J1914.7+1012 gam 19 14 43.2 +10 12 53           ~ 4 0
18 NAME Cyg X Cld 20 28 41 +41 10.2           ~ 793 1

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2023.09.28-10:36:08

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