2002ApJ...575..201R


Query : 2002ApJ...575..201R

2002ApJ...575..201R - Astrophys. J., 575, 201-216 (2002/August-2)

ROSAT/ASCA observations of the mixed-morphology supernova remnant W28.

RHO J. and BORKOWSKI K.J.

Abstract (from CDS):

We present three sets of ROSAT Position Sensitive Proportional Counter and four sets of ASCA observations of the supernova remnant (SNR) W28. The overall shape of X-ray emission in W28 is elliptical, dominated by a centrally concentrated interior emission, sharply peaked at the center. There are also partial northeastern and southwestern shells, and both the central and shell X-ray emission is highly patchy. The ASCA spectra reveal emission lines of Ne, Mg, Si, and Fe Kα and continuum extending at least up to 7 keV, showing that X-ray emission in W28 is mostly of thermal origin with a hot thermal component. We found that spectral variations are present in W28. The southwestern shell can be fitted well by a plane-shock model with a temperature of 1.5 keV and an ionization timescale of 1.5x1011 cm–3.s. The long ionization timescale combined with a low estimated electron density of ∼0.2 cm–3 imply an SNR age of several times 104 yr. The low density in the southwest is consistent with the shock breakout away from molecular clouds in the north and northeast. The northeastern shell, with a lower temperature of 0.56 keV and a longer ionization timescale of 1.7x1013 cm–3.s, spatially coincides with the radiative shell delineated by radio and optical filaments, but a relatively high temperature and a low density of X-ray-emitting gas in the northeastern shell indicate that we are not observing gas cooling from high temperatures. Unlike for the southwestern and northeastern shells, the central emission cannot be fitted well by a single-temperature model, but two components with temperatures of 0.6 and 1.8 keV are required. The long ionization timescales imply that the gas is close to the ionization equilibrium. The low-temperature component is similar to those seen in other mixed-morphology SNRs. The X-ray luminosity of W28 is ∼6x1034 ergs.s–1, and the estimated X-ray mass is only ∼20-25 M☉. A comparison of W28 with other typical mixed-morphology SNRs reveals significant differences in its X-ray properties; W28 has a higher temperature and noticeable spectral variations. W28 belongs to a class of SNRs considered by Chevalier, with a radiative shell interacting with clumpy molecular clouds. X-ray emission at its center is a ``fossil'' radiation from gas that was shocked early in the evolution of the remnant, and its centrally peaked morphology could have been caused by processes such as evaporation, electron thermal conduction, and mixing induced by various hydrodynamical instabilities, but W28 poses a challenge for existing models of X-ray emission because the evaporation model of White & Long is in conflict with observations, while the presence of temperature variations seems inconsistent with SNR models with efficient thermal conduction.

Abstract Copyright: ∼

Journal keyword(s): ISM: Individual: Alphanumeric: W28 - ISM: Supernova Remnants - X-Rays: ISM

CDS comments: p.211 : Northern source (East of the remnant) = RX J1802.1-2333

Simbad objects: 25

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Number of rows : 25
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 G132.6+01.5 SNR 02 17 40 +62 45.0           ~ 193 0
2 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
3 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
4 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1314 1
5 NAME Vela SNR 08 34.0 -45 50           ~ 1331 2
6 NAME MSH 11-61A SNR 10 59 25.36 -61 18 42.6           ~ 187 0
7 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1407 1
8 SNR G327.4+00.4 SNR 15 48 20 -53 49.0           ~ 97 0
9 SNR G359.1-00.5 SNR 17 45 30 -29 57.0           ~ 179 1
10 NAME Sgr A East SNR 17 45 41 -29 00.8           ~ 523 2
11 HD 313524 * 17 58 37.094 -23 50 52.55   11.61 11.11     A2 5 0
12 SNR G006.4-00.1 SNR 18 00 31.2011719 -23 25 48.001099           ~ 782 1
13 PSR B1758-23 Psr 18 01 19.8149 -23 04 44.630           ~ 153 0
14 CD-23 13795 * 18 01 59.5108924944 -23 39 32.745519972     11.3     A2 12 0
15 BFS 1 HII 18 01 59.7 -23 41 21           ~ 4 0
16 RX J1802.1-2333 X 18 02 10 -23 33.6           ~ 1 0
17 M 20 OpC 18 02 42 -22 58.3           ~ 456 1
18 SNR G031.9+00.0 SNR 18 49 16.3 -00 55 01           ~ 368 2
19 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 1034 2
20 SNR G053.6-02.2 SNR 19 38.8 +17 14           ~ 152 0
21 SNR G068.8+02.6 SNR 19 52 55 +32 54.2           ~ 361 1
22 SNR G082.2+05.3 SNR 20 19.0 +45 30           ~ 101 0
23 SNR G089.0+04.7 SNR 20 45.0 +50 35           ~ 237 0
24 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1
25 CTB 1 SNR 23 59 13 +62 26.2           ~ 173 0

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