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Поисковые слова: arp 220
SWIFT /XRT FOLLOW-UP OBSERVATIONS OF INTEGRAL AGNS
R. Landi, A. Malizia, L.Bassani, N. Masetti, J.B. Stephen, F.Gianotti, F. Schiavone 1 , A. Bazzano, P. Ubertini 2 , A. J. Bird, A. J. Dean3 , and R. Walter4 IASF-INAF, Bologna, Italy 2 IASF- INAF, Roma, Italy 3 University of Southampton, Southampton, UK INTEGRAL Science Data Centre, Versoix, Switzerland
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ABSTRACT In five years of operation, data from INTEGRAL has been used to discover a large number of gamma-ray sources, a substantial fraction of which have turned out to be active galactic nuclei (AGN). Recently Bassani et al. (2006) [1] have presented a sample of around 60 AGNs of which some still lack optical identification or information in the X-ray band. In this work we present X-ray data for 8 objects acquired with the XRT telescope on-board Swift satellite. The XRT positioning has allowed us to identify the optical counterparts and to classify their types through follow-up measurements. Analysis of these data has also provided information on their spectra below 10 keV. Key words: AGNs, X-rays, gamma-rays.

too crowded) to allow an optical follow-up observation. Therefore we have searched in the Swift X-Ray Telescope (XRT) [5] archive for X-ray observations of newly detected IBIS sources in order to locate them with arcsec accuracy; this us allowed their optical classification in many cases (see [7, 8, 9, 10, 11]). In this work we present X-ray data (0.2­10 keV) for a set of 8 identified with AGN.

2. SPECTRAL ANALYSIS The XRT data reduction was performed using the XRTDAS v. 2.4 standard data pipeline package (X RTP I P E L I N E v. 0.10.3), in order to produce screened event files. All data are extracted only in the Photon Counting (PC) mode [6], adopting the standard grade filtering (0­12 for PC) according to the XRT nomenclature. Events for spectral analysis were extracted within a circular region of radius 20 , which encloses about 90% of the PSF at 1.5 keV [12] centered on the source position. The background was extracted from various source-free regions close to the X-ray object of interest using both circular and annular regions of various radii, in order to ensure an evenly sampled background. In all cases, the spectra were extracted from the corresponding event files using X S E L E C T software and binned using G R P P H A in a manner so that the 2 statistic could reliably be used. We used the latest version (v.008) of the response matrices and created individual ancillary response files (ARF) using X RT M K A R F. Spectral analyses were performed using XSPEC version 12.2.1. In figures 1 to 8 we show the XRT 0.3­10 keV images for the eight new AGNs discovered by INTEGRAL together with their relative X-ray spectra. In each XRT field of view the INTEGRAL error (black circle) is shown. For those sources with more than one pointing (see label star in the table), we performed the spectral analysis of each observation individually in order to search for spectral variability, and then we analyzed the combined spectra, sa as to improve the statistical quality of the data. For this preliminary analysis, due to the limited spectral signal often available, we employed a simple power law absorbed by both a Galactic [4] and an intrinsic column

1. INTRODUCTION Our knowledge of the hard X-ray sky has been widened thanks to the capabilities of IBIS [14], the gamma-ray imager on board the INTEGRAL satellite [15]. Since its launch in October 2002, INTEGRAL has surveyed a large fraction of the sky above 20 keV at a mCrab sensitivity level with a typical localization accuracy of 2­ 3 [3]. The number of hard X-ray sources detected in the second IBIS survey has increased by 70% compared to the first one for a total of 209 objects [2, 3]. The main category (50% of the sample) is still represented by galactic accreting binaries (HMXB and LMXB), although there has been a five-fold increase in AGN detections over the 1st catalogue while the number of unclassified objects has doubled as a direct consequence of a wider and deeper sky coverage. Masetti and co-authors [7, 8, 9, 10, 11] are currently executing a campaign with the goal of identifying the still unknown sources through optical spectroscopy. Their results indicate that half of the unidentified INTEGRAL sources turn out to be optically classified as nearby AGNs. The INTEGRAL error box associated with the hard X-ray sources (2­3 ) is often too large (and therefore


Table 1. Spectral analysis of the sample Source IGR IGR IGR IGR IGR IGR IGR IGR J07597­3842 J12415­5750 J14492­5535 J16482­3036 J16558­5203 J17488­3253 J20187+4041 J20286+2544 Type Sey 1.2 Sey 2 unclas. Sey 1 Sey 1.2 Sey 1 ? unclas. SB/Sey 2 N H Gal (1021 cm-2 ) 0.630 0.346 0.500 0.176 0.304 0.530 11.9 0.261 NH (10 cm-2 ) <0.05 <0.11 10.1 +6.3 -4.3 0.13 +0.05 -0.13 <0.011 0.22 +0.07 -0.05 19.3 +20.9 -11.6 42.3 +19.5 -28.5
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1.80 +0.05 -0.03 1.70 +0.13 -0.11 F IX

1.8 1.71+0.11 -0.09 1.85 +0.06 -0.04 1.60+0.13 -0.10 1.8F I X 1.8F I X

Flux (2­10 keV) (10-12 erg cm-2 s- 22.0 8.1 2.1 10.0 18.0 14.0 1.8 2.3

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density. Due to the low statistical quality of the data, in the case of IGR J14492­5535, IGR J20187+4041 and IGR J20286+2544 we fixed the photon index to a canonical AGN value (=1.8). This baseline model provides a quite good fit to the X-ray data for all the AGNs herein analyzed and the spectral parameters obtained for each source are reported in table 1.

REFERENCES [1] Bassani, L., Molina, M., Malizia, A., Stephen, J. B., Bird, A. J., et al. 2006, ApJ 636, 65L [2] Bird, A.J., Barlow, E. J., Bassani, L., Bazzano, A., Bodaghee, A., Capitanio, F., Cocchi, M., Del Santo, M., Dean, A. J., Hill, A. B., et al. 2004, ApJ, 607, L33 [3] Bird et al. (2006)]bi06 Bird, A.J., Barlow, E.J., Bassani, L., et al. 2006, ApJ, 636, 76 [4] Dickey, J. M., & Lockman, F. J. 1990, ARA&A, 28, 215 [5] Gehrels, N., Chincarini, G., Giommi, P., et al. 2004, ApJ, 611, 1005 [6] Hill, J. E., Burrows, D. N., Nousek, J. A., et al. 2004, Proc. SPIE, 5165, 21 [7] Masetti, N., Palazzi, E., Bassani, L., Malizia, A., & Stephen, J.B. 2004, A&A, 426, L4 [8] Masetti, N., Mason, E., Bassani, L., et al. 2006a, A&A, 448, 547 [9] Masetti, N., Pretorius, M.L., Palazzi, E., et al. 2006b, A&A, 449, 1139 [10] Masetti, N., Bassani, L., Bazzano, A., et al. 2006c, A&A, 455, 11 [11] Masetti, N., Morelli, L., Palazzi, E., et al. 2006d, A&A, in press [astro-ph/0608394] [12] Moretti, A., Campana, S., Tagliaferri, G., et al. 2004, Proc. SPIE, 5165, 232 [13] Revnivtsev, M. G., Sazonov, S. Yu., Molkov, S. V., Lutovinov, A. A., et al. 2006, AstL, 32, 145 [14] Ubertini, P., Lebrun, F., Di Cocco, G., et al. 2003, A&A, 411, L131 [15] Winkler, C., Courvoisier, T.J.-L., Di Cocco, G., et al. 2003, A&A, 411, L1

3. CONCLUSIONS

The use of Swift/XRT data has allowed us to characterize the X-ray emission of eight sources presented here: for four objects the X-ray data confirm their optical classification as Seyfert 1 galaxies since no intrinsic absorption is found and the spectra are typical of AGN. For IGR J20286+2544 the intrinsic column density is compatible with a type 2 galaxy, confirming again the optical classification. It is likely that this is a Compton thick AGN ([11]), as also suggested by the presence of an excess at around 6.4 keV modelled with a narrow iron line having an equivalent width (EW) of about 700 eV. Two sources of this sample are still not optically classified (IGR J14492­5535 and IGR J20187+4041) and they are both absorbed in X-rays, suggesting a type 2 classification. IGR J12415­5750 is a peculiar source as it is a type 2 Seyfert galaxy showing no intrinsic absorption.

4. ACKNOWLEDGEMENTS

This research was supported by ASI under contract I/R/046/04 and I/R/023/05. This research has made use of data obtained from NED (Jet Propulsion Laboratory, California Institute of Technology), SIMBAD (CDS, Strasbourg, France) and HEASARC (NASA's Goddard Space Flight Center).



t

Figure 1. XRT 0.3­10 keV image with the associated INTEGRAL error box (black circle) and the corresponding XRT spectrum of all the 8 AGN presented. For IGR J14492­5535, the error boxes, corresponding to the INTEGRAL position as given by [1] (black continuum circle) and [13](black dashed circle) are plotted. The images show that for each ISGRI source an X-ray counterpart is always identified.