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Issue A&A
Volume 384, Number 1, March II 2002
Page(s) 99 - 111
Section Extragalactic astronomy
DOI http://dx.doi.org/10.1051/0004-6361:20020026



A&A 384, 99-111 (2002)
DOI: 10.1051/0004-6361:20020026

X-ray sources in the starburst spiral galaxy M 83

Nuclear region and discrete source population
R. Soria1, 2 and K. Wu1, 2

1  Mullard Space Science Laboratory, University College London, Holmbury St Mary, Surrey RH5 6NT, UK
    e-mail: kw@mssl.ucl.ac.uk
2  School of Physics A28, University of Sydney, NSW 2006, Australia

(Received 18 October 2001 / Accepted 4 January 2002 )

Abstract
Chandra has resolved the starburst nuclear region of the face-on grand-design spiral M 83. Eighty-one point sources are detected (above 3.5- $\sigma$) in the ACIS S3 image, and 15 of them are within the inner 16´´ region of the galaxy. A point source with $L_{\rm x} \approx 3 \times 10^{38}$ erg s -1 in the 0.3-8.0 keV band is found to coincide with the infra-red nuclear photometric peak, one of the two dynamical nuclei of the galaxy. No point-like sources are resolved (at a 2.5- $\sigma$ level) at the centre of symmetry of the outer optical isophote ellipses, suspected to be another dynamical nucleus. About 50% of the total emission in the nuclear region is unresolved; of this, about 70% can be attributed to hot thermal plasma, and the rest is probably due to unresolved point sources (e.g., faint X-ray binaries). The azimuthally-averaged radial distribution of the unresolved emission has a King-like profile, with no central cusp. Strong emission lines are seen in the spectrum of the optically thin plasma component. The high abundances of C, Ne, Mg, Si and S with respect to Fe suggest that the interstellar medium in the nucleus is enriched and heated by type-II supernova explosions and winds from massive stars. The cumulative luminosity distribution of the discrete X-ray sources is neither a single nor a broken power law. Separating the sources in the nuclear region (within a distance of 60´´ from the X-ray centre) from the rest reveals that the two groups have different luminosity distributions. The $\log N({>}S) - \log S$ curve of the sources in the inner region (nucleus and stellar bar) is a single power law, which we interpret as due to continuous, ongoing star formation. Outside the central region, there is a smaller fraction of sources brighter than the Eddington limit for an accreting neutron star.


Key words: galaxies: individual: M 83 (= NGC 5236) -- galaxies: nuclei -- galaxies: spiral -- galaxies: starburst -- X-rays: binaries -- X-rays: galaxies

Offprint request: R. Soria, rs1@mssl.ucl.ac.uk

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© ESO 2002


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