Abstract

The bright Seyfert 1 galaxy Mrk 509 was monitored by XMM-Newton and other satellites in 2009 to constrain the location of the outflow. We have studied the response of the photoionised gas to changes in the ionising flux produced by the central regions. We used the 5 discrete ionisation components A-E detected in the time-averaged spectrum taken with the RGS. Using the ratio of fluxed EPIC and RGS spectra, we put tight constraints on the variability of the absorbers. Monitoring with the Swift satellite started 6 weeks before the XMM-Newton observations, allowing to use the ionising flux history and to develop a model for the time-dependent photoionisation. Components A and B are too weak for variability studies, but the distance for component A is known from optical imaging of the [O III] line to be ~3 kpc. During the 5 weeks of the XMM-Newton observations we found no evidence of changes in the 3 X-ray dominant ionisation components C-E, despite a huge soft X-ray intensity increase of 60% in the middle of our campaign. This excludes high-density gas close to the black hole. Instead, using our time-dependent modelling, we find low density and derive firm lower limits to the distance of these components. Component D shows evidence for variability on longer time scales, yielding an upper limit to the distance. For component E we derive an upper limit to the distance based on the argument that the thickness of the absorbing layer must be less than its distance to the black hole. Combining these results, at the 90% confidence level, component C has a distance of >70 pc, component D between 5-33 pc, and component E >5 pc but smaller than 21-400 pc, depending upon modelling details. These results are consistent with the upper limits from the HST/COS observations of our campaign and point to an origin of the dominant, slow (v<1000 km/s) outflow components in the NLR or torus-region of Mrk 509.

Highlights

  • It has been known for a long time that accretion onto a supermassive black hole plays a key role in the physics of active galactic nuclei (AGN)

  • For component E we derive an upper limit to the distance based on the argument that the thickness of the absorbing layer must be less than its distance to the black hole

  • Key words. galaxies: active – X-rays: general – X-rays: galaxies – galaxies: individual: Mrk 509 – quasars: absorption lines

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Summary

VIII. Location of the X-ray absorber

J. S. Kaastra1,2, R. G. Detmers1,2, M. Mehdipour3, N. Arav4, E. Behar5, S. Bianchi6, G. Branduardi-Raymont3, M. Cappi7, E. Costantini1, J. Ebrero1, G. A. Kriss8,9, S. Paltani10, P.-O. Petrucci11, C. Pinto1, G. Ponti12, K. C. Steenbrugge13,14, and C. P. de Vries1

Introduction
Fluxed spectra
EPIC pn spectra
EPIC MOS spectra
RGS spectra
Description of the outflow and analysis method
Ionisation structure of the outflow
Transmission of the five components
Measuring transmission changes of the outflow
Searching for variations in the outflow in the high density limit
Ionising continuum
Predicted and observed changes in transmission: pn
Nominal significance of the variations
Predicted and observed changes in transmission
Time-dependent SEDs
Solution of the time-dependent rates
An illustrative example
Time evolution for the most prominent ions
Changes in the transmission
Long-term variability
Discussion and conclusions
Full Text
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