2017ApJ...845...48S


Query : 2017ApJ...845...48S

2017ApJ...845...48S - Astrophys. J., 845, 48-48 (2017/August-2)

Is HESS J1912+101 associated with an old supernova remnant?

SU Y., ZHOU X., YANG J., CHEN Y., CHEN X., GONG Y. and ZHANG S.

Abstract (from CDS):

HESS J1912+101 is a shell-like TeV source that has no clear counterpart in multiwavelength. Using CO and H I data, we reveal that VLSR ∼ +60 km s–1 molecular clouds (MCs), together with shocked molecular gas and high-velocity neutral atomic shells, are concentrated toward HESS J1912+101. The prominent wing profiles up to VLSR ∼ +80 km s–1 seen in 12CO (J = 1-0 and J = 3-2) data, as well as the high-velocity expanding H I shells up to VLSR ∼ +100 km s–1, exhibit striking redshifted-broadening relative to the quiescent gas. These features provide compelling evidences for large-scale perturbation in the region. We argue that the shocked MCs and the high-velocity H I shells may originate from an old supernova remnant (SNR). The distance to the SNR is estimated to be ∼4.1 kpc based on the H I self-absorption method, which leads to a physical radius of 29.0 pc for the ∼(0.7-2.0) x 105 years old remnant with an expansion velocity of >=40 km s–1. The +60 km s–1 MCs and the disturbed gas are indeed found to coincide with the bright TeV emission, supporting the physical association between them. Naturally, the shell-like TeV emission comes from the decay of neutral pions produced by interactions between the accelerated hadrons from the SNR and the surrounding high-density molecular gas.

Abstract Copyright: © 2017. The American Astronomical Society. All rights reserved.

Journal keyword(s): ISM: individual objects: shell-like clouds, HESS J1912+101 - ISM: kinematics and dynamics - ISM: supernova remnants - ISM: supernova remnants

Simbad objects: 6

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Number of rows : 6
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 ARGO J1912+1026 gam 19 12 14.9 +10 21 06           ~ 51 0
2 [MCM2005b] 20 OpC 19 12 25 +09 57.7           ~ 17 0
3 2HWC J1912+099 gam 19 12.4 +09 56           ~ 5 0
4 PSR J1913+1000 Psr 19 13 03.59 +10 00 02.4           ~ 18 0
5 PSR J1913+1011 Psr 19 13 20.341 +10 11 22.97           ~ 84 0
6 HRDS G044.528-00.234 HII 19 13 39.9 +10 11 49           ~ 5 0

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