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arXiv · 1803.07334

Multi-wavelength campaign on NGC 7469 IV. The broad-band X-ray spectrum

Abstract

We conducted a multi-wavelength six-month campaign to observe the Seyfert galaxy NGC~7469, using the space-based observatories \textit{HST}, \textit{Swift}, \textit{XMM-Newton} and \textit{NuSTAR}. Here we report the results of the spectral analysis of the 7 simultaneous \textit{XMM-Newton} and \textit{NuSTAR} observations. The sources shows significant flux variability within each observation, but the average flux is less variable among the different pointings of our campaign. Our spectral analysis reveals a prominent narrow neutral \ion{Fe} K$\alpha$ emission line in all the spectra, with weaker contributions from Fe K$\beta$, neutral Ni K$\alpha$ and ionised iron. We find no evidence for variability or relativistic effects acting on the emission lines, which indicates that they originate from distant material. Analysing jointly \textit{XMM-Newton} and \textit{NuSTAR} data a constant photon index is found ($\Gamma$=$1.78\pm0.02$), together with a high energy cut-off $E_{\rm{cut}}=170^{+60}_{-40}$ keV. Adopting a self-consistent Comptonization model, these values correspond to an average coronal electron temperature of kT=$45^{+15}_{-12}$ keV and, assuming a spherical geometry, an optical depth $\tau=2.6\pm0.9$. The reflection component is consistent with being constant, with a reflection fraction in the range $R=0.3-0.6$. A prominent soft excess dominates the spectra below 4 keV. This is best fit with a second Comptonization component, arising from a \virg{warm corona} with an average $kT=0.67\pm0.03$ keV and a corresponding optical depth $\tau=9.2\pm0.2$.

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R. Middei, S. Bianchi, M. Cappi, P-O. Petrucci, F. Ursini, N. Arav, E. Behar, G. Branduardi-Raymont, E. Costantini, B. De Marco, L. Di Gesu, J. Ebrero, J. Kaastra, S. Kaspi, G. A. Kriss, J. Mao, M. Mehdipour, S. Paltani, U. Peretz, G. Ponti. 2018-03-20. Multi-wavelength campaign on NGC 7469 IV. The broad-band X-ray spectrum. https://doi.org/10.1051/0004-6361%2F201832726

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