2013ApJ...779..179P


Query : 2013ApJ...779..179P

2013ApJ...779..179P - Astrophys. J., 779, 179 (2013/December-3)

Fermi LAT and WMAP observations of the supernova remnant HB 21.

PIVATO G., HEWITT J.W., TIBALDO L., ACERO F., BALLET J., BRANDT T.J., DE PALMA F., GIORDANO F., JANSSEN G.H., JOHANNESSON G. and SMITH D.A.

Abstract (from CDS):

We present the analysis of Fermi Large Area Telescope γ-ray observations of HB 21 (G89.0+4.7). We detect significant γ-ray emission associated with the remnant: the flux >100 MeV is 9.4±0.8 (stat)±1.6 (syst)x10–11 erg/cm2/s. HB 21 is well modeled by a uniform disk centered at l = 88.°75±0.°04, b = +4.°65±0.°06 with a radius of 1.°19±0.°06. The γ-ray spectrum shows clear evidence of curvature, suggesting a cutoff or break in the underlying particle population at an energy of a few GeV. We complement γ-ray observations with the analysis of the WMAP 7 yr data from 23 to 93 GHz, achieving the first detection of HB 21 at these frequencies. In combination with archival radio data, the radio spectrum shows a spectral break, which helps to constrain the relativistic electron spectrum, and, in turn, parameters of simple non-thermal radiation models. In one-zone models multiwavelength data favor the origin of γ rays from nucleon-nucleon collisions. A single population of electrons cannot produce both γ rays through bremsstrahlung and radio emission through synchrotron radiation. A predominantly inverse-Compton origin of the γ-ray emission is disfavored because it requires lower interstellar densities than are inferred for HB 21. In the hadronic-dominated scenarios, accelerated nuclei contribute a total energy of ∼3x1049 erg, while, in a two-zone bremsstrahlung-dominated scenario, the total energy in accelerated particles is ∼1x1049 erg.

Abstract Copyright: ∼

Journal keyword(s): acceleration of particles - cosmic rays - ISM: individual: HB 21 - radiation mechanisms: non-thermal

Simbad objects: 26

goto Full paper

goto View the references in ADS

Number of rows : 26
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 SNR G130.7+03.1 SNR 02 05 35.73 +64 49 41.3           ~ 661 4
2 SNR G180.0-01.7 SNR 05 39 00.000 +27 50 00.00           ~ 294 2
3 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1314 1
4 SNR G006.4-00.1 SNR 18 00 31.2011719 -23 25 48.001099           ~ 782 1
5 SNR G031.9+00.0 SNR 18 49 16.3 -00 55 01           ~ 368 2
6 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 1034 2
7 W 49b SNR 19 11 09.5 +09 06 21           ~ 500 1
8 SNR G049.1-00.1 SNR 19 23 19.300 +14 09 21.00           ~ 309 0
9 ICRF J202939.8+492622 Bla 20 29 39.87459383 +49 26 22.1476662           ~ 45 1
10 NAME Cyg X Cld 20 30 04.7973633 +40 51 36.002197           ~ 962 1
11 NAME Cyg Complex reg 20 32 +45.0           ~ 667 0
12 3C 418.0 Bla 20 38 37.03472279 +51 19 12.6624988   21.30 21.00 18.9   ~ 333 1
13 RX J2039.3+5219 BLL 20 39 23.5181915742 +52 19 50.035414651     19.0 16.2   ~ 84 1
14 2FGL J2041.2+4735 gam 20 41 17.3 +47 35 38           ~ 17 0
15 2FGL J2041.5+5003 gam 20 41 30 +50 04.0           ~ 7 0
16 2FGL J2043.3+5105 gam 20 43 21 +51 05.9           ~ 7 0
17 SNR G089.0+04.7 SNR 20 45.0 +50 35           ~ 237 0
18 PSR J2047+5029 Psr 20 47 54.640 +50 29 38.17           ~ 18 0
19 NAME Cyg Loop SNR 20 51.0 +30 40           ~ 964 0
20 2FGL J2051.8+5054 gam 20 51 45.4 +50 51 10           ~ 10 0
21 2FGL J2055.8+4754 gam 20 55 52.1 +47 54 32           ~ 6 0
22 2MASS J20564271+4940068 BLL 20 56 42.7402786032 +49 40 06.604076316           ~ 79 1
23 ICRF J210217.0+470216 BLL 21 02 17.05602493 +47 02 16.2532939           ~ 70 1
24 Ass Cyg OB 7 As* 21 08 +47.6           ~ 218 0
25 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1
26 NAME Local Arm reg ~ ~           ~ 649 0

To bookmark this query, right click on this link: simbad:objects in 2013ApJ...779..179P and select 'bookmark this link' or equivalent in the popup menu