Confirmation of the nature of the absorber in IRAS 09104+4109

TL;DR

This study uses Suzaku and Chandra X-ray data to determine that IRAS 09104+4109 is a Compton-thin AGN, clarifying its absorber nature and resolving previous contamination issues from nearby sources.

Contribution

First simultaneous soft and hard X-ray observations of IRAS 09104+4109 clarify its Compton-thin nature, resolving previous ambiguities caused by contamination and model degeneracies.

Findings

IRAS 09104+4109 is a Compton-thin AGN with N_H ~ 5 x 10^23 cm^-2

The iron line is a blend, with 6.4 keV from the AGN and 6.7 keV from hot gas

Reflection model is more likely due to the iron line analysis

Abstract

We present the first long \emph{Suzaku} observation of the hyperluminous infrared galaxy IRAS 09104+4109 which is dominated by a Type 2 AGN. The infrared to X-ray SED indicates that the source is an obscured quasar with a Compton-thin absorber. However, the 3$\sigma$ hard X-ray detection of the source with the \emph{BeppoSAX} PDS suggested a reflection-dominated, Compton-thick view. The high-energy detection was later found to be possibly contaminated by another Type 2 AGN, NGC 2785, which is only 17 arcmin away. Our new \emph{Suzaku} observation offers simultaneous soft and hard X-ray coverage and excludes contamination from NGC 2785. We find that the hard X-ray component is not detected by the \emph{Suzaku} HXD/PIN (effective energy band 14-45 keV). Both reflection and transmission models have been tested on the latest \emph{Suzaku} and \emph{Chandra} data. The 0.5-10 keV spectrum can be well modelled by the two scenarios. In addition, our analysis implied that the absorption column required in both models is $N_{\rm H} \sim 5 \times 10^{23}$ cm$^{-2}$. Unless IRAS 09104+4109 is a "changing-look" quasar, we confirm that it is a Compton-thin AGN. Although the lack of detection of X-ray emission above 10 keV seems to favour the transmission scenario, we found that the two models offer fairly similar flux predictions over the X-ray band below $\sim$ 40 keV. We also found that the strong iron line shown in the \emph{Suzaku} spectrum is in fact a blend of two emission lines, in which the 6.4 keV one is mostly contributed from the AGN and the 6.7 keV from the hot cluster gas. This implies that the neutral line is perhaps caused by disc reflection, and the reflection-dominated model is more likely the explanation. The transmission model should not be completely ruled out, but a deeper hard X-ray spectrum observation is needed to discriminate between the two scenarios.