1998A&A...329...39E


Query : 1998A&A...329...39E

1998A&A...329...39E - Astronomy and Astrophysics, volume 32939-54 (1998/1-1)

ROSAT PSPC X-ray observations of the nearby spiral galaxy M 83.

EHLE M., PIETSCH W., BECK R. and KLEIN U.

Abstract (from CDS):

The nearly face-on SBc galaxy M 83 (NGC 5236) was observed for 25 ksec with the ROSAT PSPC. We detected 13 point-like sources in this galaxy, 10 of which were previously unknown, down to a limiting luminosity of ∼0.8x1038erg/s (for D=8.9Mpc). Eight of these sources are positionally associated with HII regions and/or HI voids, suggesting an association with the younger stellar population, variable X-ray binaries or with hot expanding gaseous bubbles. We measured extended X-ray radiation from almost the whole optically visible galaxy with a luminosity of Lx∼3.6x1040erg/s in the energy range 0.1-2.4keV. Approximately 20% of this emission can be explained by undetected point-like sources. We detected diffuse soft (0.1-0.4keV) X-ray emission due to hot gas with a luminosity of Lx(soft)∼1.4x1040erg/s. Comparing the diffuse soft and hard X-ray emission components, we observed a different asymmetric distribution and a slower radial decrease of the intensity profile of the soft X-ray emission. Both these results support the existence of a huge spherical gas halo of ∼10-15kpc radius. On the other hand, the radial scale lengths of the hard X-ray radiation, that of the thermal radio emission and the profile of the optical surface brightness are similar, favouring the idea that all these emission processes are connected to star formation in the galaxy's disk. M 83 is the first face-on galaxy where the diffuse X-ray emission spectrum can be characterized by a two-temperature thermal plasma: a soft X-ray emitting warm `halo component' of plasma temperature 2.1x106K and an internally absorbed hot `disk component' at 5.7x106K which is dominating the emission in the hard (0.5-2.0keV) ROSAT energy range. The (distance-independent) mean surface brightness of the soft diffuse emission of M 83 is about twice that of NGC 253. The electron densities in the galactic halo of M 83 (∼1.2x10–3/sqrt(η)cm–3, with a volume filling factor η) are in general too low to explain the observed depolarization of the radio emission. This indicates that the ionization equilibrium might be violated, leading to higher electron densities. The combination of X-ray and radio polarization observations allows an estimate of the plasma parameter β=Utherm/Umagn which is found to be 0.2±0.1. This result supports the hypothesis that magnetic fields play an important role for the evolution and structure of galactic gas haloes. The high energy input rate in the active star-forming disk of M 83 seems to be responsible for the outflow of hot gas and the halo formation.

Abstract Copyright: ∼

Journal keyword(s): galaxies: individual: M 83 - haloes - ISM - magnetic fields - X-rays: galaxies

Nomenclature: Table 4: [EPB98] NN (Nos 1-47)

Simbad objects: 66

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Number of rows : 66
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 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
2 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3588 2
3 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
4 NGC 1808 Sy2 05 07 42.343 -37 30 46.98 11.05 10.80 9.94 9.36 10.2 ~ 756 3
5 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
6 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
7 NGC 3628 LIN 11 20 17.018 +13 35 22.16   10.42 9.48 9.22   ~ 853 3
8 NGC 4565 Sy2 12 36 20.804 +25 59 14.61   13.61 12.43     ~ 991 0
9 NGC 4631 GiC 12 42 08.009 +32 32 29.44   9.78 9.19 9.10   ~ 1154 3
10 M 51 Sy2 13 29 52.698 +47 11 42.93   9.26 8.36 8.40   ~ 4565 4
11 1RXS J133530.6-295031 BLL 13 35 29.7518919576 -29 50 38.921848188   18.13   19.25   ~ 70 0
12 RX J133543-29501 X 13 35 43.3 -13 35 44           ~ 1 0
13 RX J133548-29563 X 13 35 49.0 -29 56 21           ~ 1 0
14 RX J133611-29435 X 13 36 11.9 -29 43 32           ~ 1 0
15 RX J133614-29560 X 13 36 14.4 -29 56 03           ~ 1 0
16 RX J133615-29578 G 13 36 15.6 -29 57 51           ~ 2 0
17 RX J133618-30013 X 13 36 18.9 -30 01 23           ~ 1 0
18 RX J133619-29346 X 13 36 19.0 -29 34 38           ~ 1 0
19 RX J133627-29555 X 13 36 27.8 -29 55 34           ~ 1 0
20 RX J133633-30034 X 13 36 33.7 -30 03 29           ~ 1 0
21 RX J133639-29476 X 13 36 39.5 -29 47 39           ~ 1 0
22 RX J133641-29598 X 13 36 41.1 -29 59 48           ~ 1 0
23 RX J133644-29509 X 13 36 43.53 -29 51 06.9           ~ 9 0
24 6dFGS gJ133645.8-295913 G 13 36 45.8159805984 -29 59 12.551439912   17.15   15.66 15.02 ~ 10 0
25 RX J133645-30033 X 13 36 46.0 -30 03 18           ~ 1 0
26 RX J133646-29519 X 13 36 46.6 -29 51 55           ~ 2 0
27 RX J133649-29527 X 13 36 49.8 -29 52 47           ~ 4 1
28 SN 1983N SN* 13 36 51.23 -29 54 01.7   11.7       SNIb 278 1
29 SN 1950B SN* 13 36 52.88 -29 51 55.7   14.5 14.5     ~ 58 1
30 RX J133658-29435 X 13 36 58.9 -29 43 31           ~ 1 0
31 RX J133659-29499 X 13 36 59.85 -29 49 55.5           ~ 3 0
32 SN 1968L SN* 13 37 00.42 -29 51 59.8   12.0 12.0     SNIIP 83 1
33 RX J133700-29518 X 13 37 00.8 -29 51 50           ~ 2 0
34 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2778 2
35 RX J133701-29534 LXB 13 37 01.48 -29 53 26.5           ~ 12 0
36 SN 1957D SN* 13 37 03.57 -29 49 40.7   15.0 15.0     ~ 121 1
37 RX J133704-29539 HXB 13 37 04.28 -29 54 03.6           ~ 13 0
38 RX J133704-29513 X 13 37 04.3 -29 51 20           ~ 3 1
39 RX J133705-29529 X 13 37 05.9 -29 52 56           ~ 3 0
40 RX J133707-29508 X 13 37 07.3 -29 50 51           ~ 1 0
41 SN 1923A SN* 13 37 09.2 -29 51 04   12.4 14.0     SNIIP: 80 1
42 RX J133711-29356 X 13 37 11.4 -29 35 40           ~ 1 0
43 RX J133715-30027 X 13 37 15.5 -30 02 43           ~ 1 0
44 RX J133716-29495 X 13 37 16.38 -29 49 39.4           ~ 7 0
45 RX J133719-29536 ULX 13 37 20.12 -29 53 47.7           ~ 24 2
46 RX J133725-29588 X 13 37 25.3 -29 58 51           ~ 1 0
47 RX J133730-29425 X 13 37 30.3 -29 42 32           ~ 1 0
48 RX J133731-29518 X 13 37 31.6 -29 51 53           ~ 1 0
49 RX J133736-29482 X 13 37 36.8 -29 48 15           ~ 1 0
50 RX J133738-30033 X 13 37 38.9 -30 03 21           ~ 1 0
51 RX J133739-29433 X 13 37 39.4 -29 43 18           ~ 1 0
52 RX J133742-29515 X 13 37 42.4 -29 51 34           ~ 1 0
53 RX J113744-30057 X 13 37 44.3 -30 05 47           ~ 1 0
54 RX J133744-29529 X 13 37 44.7 -29 52 59           ~ 1 0
55 RX J133749-29566 X 13 37 49.7 -29 56 38           ~ 1 0
56 RX J133803-29439 X 13 38 03.5 -29 44 00           ~ 1 0
57 RX J133806-29576 X 13 38 06.1 -29 57 39           ~ 1 0
58 RX J133806-29443 X 13 38 06.2 -29 44 23           ~ 1 0
59 RX J133806-29436 X 13 38 06.7 -29 43 40           ~ 1 0
60 RX J133806-29452 X 13 38 06.9 -29 45 12           ~ 1 0
61 RX J133809-29576 X 13 38 09.3 -29 57 41           ~ 1 0
62 RX J133811-29539 X 13 38 11.7 -29 53 59           ~ 1 0
63 RX J133656-29481 X 13 39 46.4 -30 03 18           ~ 3 0
64 M 101 GiP 14 03 12.583 +54 20 55.50   8.46 7.86 7.76   ~ 3138 2
65 NGC 7714 AGN 23 36 14.1257730600 +02 09 18.197422668   14.91 14.36     ~ 788 1
66 APG 284 PaG 23 36 19 +02 09.3   12.6       ~ 608 0

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