High-resolution X-ray spectroscopy and imaging of Mrk 573
We present a detailed analysis of the XMM–Newton Reflection Grating Spectrometer (RGS) high-resolution X-ray spectra of the Seyfert 2 galaxy, Mrk 573. This analysis is complemented by the study of the Chandra image and its comparison to optical (Hubble Space Telescope) and radio (Very Large Array) d...
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Veröffentlicht in: | Monthly notices of the Royal Astronomical Society 2010-06, Vol.405 (1), p.553-563 |
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Sprache: | eng |
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Zusammenfassung: | We present a detailed analysis of the XMM–Newton Reflection Grating Spectrometer (RGS) high-resolution X-ray spectra of the Seyfert 2 galaxy, Mrk 573. This analysis is complemented by the study of the Chandra image and its comparison to optical (Hubble Space Telescope) and radio (Very Large Array) data. The soft X-ray emission is mainly due to gas photoionized by the central active galactic nucleus, as indicated by the detection of radiative recombination continua from O vii and O viii as well as by the prominence of the O vii forbidden line. This result is confirmed by the best fit obtained with a self-consistent cloudy photoionization model. However, a collisionally excited component is also required, in order to reproduce the Fe xvii lines, accounting for about one-third of the total luminosity in the 15–26 Å band. Once the same model in the Chandra Advanced CCD Imaging Spectrometer (ACIS) data is adopted, another photoionized component, with a higher ionization parameter, is needed to take into account emission from higher Z metals. The broad-band ACIS spectrum also confirms the Compton-thick nature of the source. The imaging analysis shows the close morphological correspondence between the soft X-ray and the [O iii] emission. The radio emission appears much more compact, although clearly aligned with the narrow-line region. The collisional phase of the soft X-ray emission may be due to starburst, requiring a star formation rate of ≃5–9 M⊙ yr−1, but there is no clear evidence of this kind of activity from other wavelengths. On the other hand, it may be related to the radio ejecta, responsible for the heating of the plasma interacting with the outflow, but the estimated pressure of the hot gas is much larger than the pressure of the radio jets, assuming equipartition and under reasonable physical parameters. |
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ISSN: | 0035-8711 1365-2966 |
DOI: | 10.1111/j.1365-2966.2010.16475.x |