2009ApJ...706L.270H


Query : 2009ApJ...706L.270H

2009ApJ...706L.270H - Astrophys. J., 706, L270-L274 (2009/December-1)

Correlation of supernova remnant masers and gamma-ray sources.

HEWITT J.W., YUSEF-ZADEH F. and WARDLE M.

Abstract (from CDS):

Supernova remnants (SNRs) interacting with molecular clouds are potentially exciting systems in which to detect evidence of cosmic ray acceleration. Prominent γ-ray emission is produced via the decay of neutral pions when cosmic rays encounter nearby dense clouds. In many of the SNRs coincident with γ-ray sources, the presence of OH (1720 MHz) masers is used to identify interaction with dense gas and to provide a kinematic distance to the system. In this Letter we use statistical tests to demonstrate that there is a correlation between these masers and a class of GeV- to TeV-energy γ-ray sources coincident with interacting remnants. For pion decay the γ-ray luminosity provides a direct estimate of the local cosmic ray density. We find the cosmic ray density is enhanced by one to two orders of magnitude over the local solar value, comparable to X-ray-induced ionization in these remnants. The inferred ionization rates are sufficient to explain non-equilibrium chemistry in the post-shock gas, where high columns of hydroxyl are observed.

Abstract Copyright:

Journal keyword(s): cosmic rays - masers - shock waves - supernova remnants

Simbad objects: 30

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Number of rows : 30
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 1FGL J0538.6+2717 BL? 05 39 00.000 +27 50 00.00           ~ 253 2
2 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1237 1
3 NAME MSH 11-61A SNR 10 59 25.36 -61 18 42.6           ~ 175 0
4 PSR J1410-6132 Psr 14 10 24.000 -61 32 00.00           ~ 128 1
5 SNR G312.4-00.4 SNR 14 13 00 -61 44.0           ~ 92 1
6 SNR G337.0-00.1 SNR 16 35 06.9 -47 47 25           ~ 131 1
7 SNR G337.8-00.1 SNR 16 39.0 -46 59           ~ 76 0
8 SNR G348.5+00.1 SNR 17 14 31.780 -38 28 34.50           ~ 220 3
9 SNR G353.6-00.7 SNR 17 31 55.0 -34 42 36           ~ 143 0
10 SNR G355.6+00.0 SNR 17 35 18 -32 37.0           ~ 27 0
11 SNR G359.1-00.5 Rad 17 45 30 -29 57.0           ~ 174 1
12 0FGL J1746.0-2900 gam 17 45 41 -29 00.8           ~ 494 2
13 NAME Sgr D SNR SNR 17 48.7 -28 07           ~ 17 0
14 SNR G005.7-00.1 SR? 17 58.8 -24 03           ~ 26 0
15 SNR G006.4-00.1 SNR 18 00 31.2011719 -23 25 48.001099           ~ 738 1
16 W 30 BL? 18 05 31.2011719 -21 25 48.001099           ~ 174 1
17 SNR G016.8-01.1 SNR 18 25.3 -14 46           ~ 38 0
18 V* V479 Sct HXB 18 26 15.0561548880 -14 50 54.247274304 12.02 12.23 11.27 11.04   ON6V((f))z 573 2
19 SNR G021.8-00.6 SNR 18 32 45 -10 08.0           ~ 129 0
20 3C 391.0 BL? 18 49 16.3 -00 55 01           ~ 352 2
21 4C -00.73 Rad 18 51 46.9 -00 03 19           ~ 100 1
22 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 965 2
23 SNR G039.2-00.3 SNR 19 04 03.9 +05 26 56           ~ 192 1
24 W 49b SNR 19 11 09.000 +09 06 24.00           ~ 463 1
25 SNR G049.1-00.1 SNR 19 23 19.300 +14 09 21.00           ~ 283 0
26 QSO J2015+371 BLL 20 15 28.72978661 +37 10 59.5147372     21.82 21.4   ~ 299 2
27 SNR G074.9+01.2 SNR 20 16 02.4 +37 12 48           ~ 182 2
28 NAME gam Cyg SNR BL? 20 20 17.100 +40 26 09.00           ~ 229 2
29 GRO J2019+40 gam 20 21.5 +40 26           ~ 129 1
30 PSR J2021+4026 Psr 20 21 30.496 +40 26 53.56           ~ 275 2

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