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X-ray luminous galaxies II. Chandra and XMM-Newton Observations of the 'composite' galaxy I_图文

X-ray luminous galaxies II. Chandra and XMM-Newton Observations of the ’composite’ galaxy IRAS20051-1117
I. Georgantopoulos1 I. Papadakis2 A. Zezas3 M. J. Ward4 ABSTRACT We present Chandra and XMM-Newton observations of the composite starforming/Seyfert galaxy IRAS20051-1117. The X-ray imaging and spectral properties reveal the presence of an active nucleus. The Chandra image shows a strong nuclear point source (L(2 ? 10keV) ? 4 × 1042 erg s?1 ). The nuclear X-ray source coincides with a bright, also un-resolved, UV source which appears in the XMMNewton Optical Monitor images. The XMM-Newton and Chandra spectrum is well represented by a power-law with a photon index of Γ ? 1.7 ? 1.9 and a thermal component with a temperature of ? 0.2 keV. We also detect an Fe line at 6.4 keV with an equivalent width of ? 0.3 keV, typical of the iron lines that have been detected in the X-ray spectra of “classical” AGN. We ?nd no evidence for short-term variability in the X-ray light curves, while we detect no variations between the XMM-Newton and Chandra observations which are separated by about 20 days. Optical spectroscopic observations which were performed ? 2.5 months after the XMM-Newton observation show that the optical spectrum is dominated by a star-forming galaxy component, although a weak broad Hα component is present, in agreement with the results from past observations. The lack of strong AGN signatures in the optical spectrum of the source can be explained by the dilution of the nuclear AGN emission by the nuclear star-forming component and the strong emission of the underlying, bright host galaxy. Subject headings: galaxies: individual (IRAS20051-1117) — galaxies: nuclei — galaxies: active — quasars: general
Institute of Astronomy & Astrophysics, National Observatory of Athens, Palaia Penteli, 15236, Athens, Greece
2 3 4 1

arXiv:astro-ph/0406286v1 11 Jun 2004

Physics Department, University of Crete, 71003, Heraklion, Greece Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA02138 X-ray Astronomy Group, Department of Physics & Astronomy, University of Leicester, LE1 7RH, UK

–2– 1. Introduction

Chandra and XMM-Newton surveys revealed the presence of a large population of ’optically inactive’ or ’passive’ galaxies (Mushotzky et al. 2000, Severgnini et al. 2003, Alexander et al. 2003, Green et al. 2004), con?rming previous ?ndings by ROSAT (Gri?ths et al. 1995, Boyle et al. 1995, McHardy et al. 1998). The optical spectra of these galaxies do not show evidence for either broad or high excitation lines (e.g. Barger et al. 2001). However, in most cases the X-ray luminosities observed are in excess of Lx ? 1042 erg s?1 which is considered as the upper limit for the X-ray emission of bona-?de star-forming galaxies (e.g. Zezas, Georgantopoulos & Ward 1998, Moran et al. 1999) suggesting the presence of active nuclei. It is possible that these galaxies represent a mixed class of objects. In the case of ’Fiore P3’, which is probably the most well studied case of the ’passive’ galaxies, Comastri et al. (2002) ?nd that it is most likely associated with an obscured AGN. Severgnini et al. (2003) ?nd instead that a number of galaxies detected in their XMM-Newton survey present X-ray spectra with no evidence for absorption. The dichotomy between the optical and X-ray classi?cation could then be explained if the galaxy light dilutes the weak nuclear component (see also Moran et al. 2002, Georgantopoulos et al. 2003 for further examples of such objects). The ’optically inactive’ galaxies bear many similarities to the ’composite’ class of objects discovered by Veron et al. (1981) and further discussed by Moran et al. (1996). The diagnostic emission line diagrams of Veilleux et al. (1995) classify these as star-forming galaxies. Yet, their X-ray luminosities usually exceed 1042 erg s?1 (Moran et al. 1996); moreover, a fraction of the ’composites’ present weak Hα broad wings. Chandra observations of the ’composite’ IRAS00317-2142 (Georgantopoulos et al. 2003) showed that the X-ray emission of this object is dominated by a variable nuclear point source which presents an unabsorbed X-ray spectrum. Here, we present XMM-Newton and Chandra observations of IRAS20051-1117. This is one of the most luminous ’composite’ objects in the Moran et al. (1996) sample, with a high, soft X-ray luminosity (in excess of 1042 erg s?1 ) at a redshift of z ≈ 0.0315. The diagnostic emission line ratios (Hα /[NII] versus Hβ /[OIII]) classify it as a star-forming galaxy (Moran et al. 1996). Nevertheless, its high X-ray luminosity as well as a faint broad Hα wing would classify this as an AGN. The excellent spatial resolution of Chandra combined with the high e?ective area and good energy resolution of the XMMNewton mission can be used to unveil the nature of the AGN which is hosted in this galaxy. Throughout this paper, we adopt a Hubble constant of Ho = 65km s?1 Mpc?1 .

–3– 2. Observations and Data Reduction 2.1. Chandra

IRAS20051-1117 was observed using the Advanced CCD Imaging Spectrometer, ACISS, onboard Chandra (Weisskopf et al. 1996). The observation date was 20 April 2002 (Sequence Number 700383). We use the cleaned event ?le provided by the standard pipeline processing having an exposure time of 20.1 ksec. Only Grade 0,2,3,4 and 6 events are used in the analysis. The whole galaxy falls on only one chip (S3). Charge Transfer Ine?ciency (CTI) problems do not a?ect our observations as S3 is back-illuminated chip. Each CCD chip subtends an 8.3 arcmin square on the sky while the pixel size is 0.5′′ . The spatial resolution on-axis is 0.5′′ FWHM. The ACIS-S spectral resolution is ?100 eV (FWHM) at 1.5 keV. We observed in 1/4-subarray mode in order to minimize pile-up problems; in this mode the size of the chip is reduced e?ectively to about 2x8 arcmin. We obtain about 7000 counts in the total 0.3-8 keV band, after background subtraction, corresponding to a count rate of 0.35 cts s?1 . Then, the PIMMS software estimates a pile-up fraction of less than 10%. Images, spectra, ancillary ?les, response matrices, and lightcurves have been created using the CIAO v2.2 software. We use a 2′′ radius extraction region in order to produce both the spectral ?les and the lightcurves. We take into account the degradation of the ACIS quantum e?ciency in low energies, due to molecular contamination, by using the ACISABS model in the spectral ?tting1 . The imaging analysis was performed using the SHERPA software.



The XMM-Newton data were obtained in 01 April 2002 as part of the Guest Observer Programme AO-1. The EPIC (European Photon Imaging Camera; Str¨ der et al. 2001 u and Turner et al. 2001) cameras were operated in full frame mode with the thin ?lter applied. The data have been cleaned and processed in the standard pipeline mode using the Science Analysis Software (sas). The event ?les for the PN and the two MOS detectors were produced using the standard reduction pipeline (Watson et al. 2001). The event ?les were screened for high particle background periods resulting in a good time interval of about 5.5 ksec for both MOS and PN. Events corresponding to patterns 0–4 and 0–12 have been included in the analysis of the PN and MOS data respectively. We obtain about 5.500 and 3500 background subtracted counts in the PN and the combined MOS respectively. The resulting count rates are ≈ 1 and 0.7 cts s?1 respectively. We use a 4 pixel (? 16′′ ) radius

http://asc.harvard.edu/cal/Acis/Cal prods/qeDeg

–4– extraction region, in order to obtain the spectrum (and the lightcurve) of our source. We obtain the background from a region from the same CCD chip with an area about 10 times larger than the source extraction region. We create the auxiliary ?les for the PN and MOS using the SAS task arfgen to take into account both instrumental e?ects (e.g. quantum e?ciency, telescope e?ective area, ?lter transmission) and the fraction of light falling outside the extraction radius. The spectral response ?les are created using the task rmfgen. Finally, during the XMM-Newton observation, the OM (Optical Monitor) was operated in Imaging mode. The source was observed with the B, UVW1 (i.e. U) and UVW2 ?lters. The total exposure time was 4, 5 and 6 ksec respectively. In the subsequent analysis we use the processed, standard pipeline mode data (which were reduced using SAS version 5.3.2).


Data Analysis 3.1. Imaging

In Fig. 1 we plot the Chandra X-ray contours in the total band (0.3-8 keV) overlayed on the XMM-Newton OM (Optical Monitor) image in the U (UVW1, 2900 ?) ?lter. All the XA ray emission emanates from the source coinciding with the optical nucleus. The coordinates of the X-ray source are α = 20h07m51.3s, δ = ?11? 08m33s (J2000); note that the IRAS name for this object refers to B1950. We have ?tted the two-dimensional spatial pro?le of the Chandra source with the SHERPA software. Fitting a Gaussian pro?le, we obtain a FWHM of 1.78 ± 0.02 pixels. Given that the nominal Point Spread Function (PSF) is undersampled by the pixels of the ACIS camera (FWHMP SF ? 0.5′′ at 1.5 keV, compared to a pixel size of 0.49′′) we consider the probability of any extension marginal. Indeed, the Gaussian ?t to the Point Spread Function generated with the CIAO mkpsf task gives a comparable FWHM (≈ 1.5 ± 0.02 pixels). Fig. 1 shows that the central UV-bright source in IRAS20051-1117 is surrounded by some faint nebulosity which is associated with the galaxy. The nuclear source appears to be point-like in the UV. In order to investigate this issue further, we co-added the 5 UVW1 and UVW2 images to create a single image. Using IRAF, we ?tted the one-dimensional radial pro?le of the central source in both ?lters with a Gaussian. The FWHM of the Gaussian pro?le is ? 2.5′′ and ? 1.8′′ in the case of the UVW1 and UVW2 images, respectively. The pro?le of the UVW1 source appears to be slightly larger than the width of the nominal PSF for this ?lter (1.7′′ ). The FWHM of the UVW2 source is identical to the PSF width for this ?lter (1.8′′ ). As the contribution of the underlying galaxy is much more pronounced in the

–5– UVW1 image, our results imply that, just like with the X-ray source, the UV source is not resolved either, its size being equal to or smaller than ? 2′′ which corresponds to ?1.4 kpc.



Fig. 2 (upper panel) shows the background subtracted PN and MOS light curves for IRAS20051-1117 in the 0.3 - 8 keV band (open squares, ?lled and open circles for PN, MOS-1 and MOS-2 light curves, respectively). The time bin size was set to 200 sec. All cameras were switched on about the same time, however there are a few gaps of duration ? 20 ? 800 sec in all light curves, due to the rejetion of periods with high particle background. The light curves appear to be ?at, with no signi?cant variations above the intrumental noise. Using the χ2 test, we ?nd that the light curves are consistent with the hypothesis of a constant ?ux. This is true even when we consider the combined, background subtracted PN and MOS light curves. The Chandra 0.3-8 keV light curve does not show any signi?cant, intrinsic variations either (Fig. 2, lower panel). We conclude that IRAS20051-1117 does not show any signi?cant variations on time scales smaller than ? 10 ksec. Next, we examine whether there is any evidence for long term variability. Using the best ?t power-law spectrum derived from the PN data (Γ = 1.94 see section 3.3 below) we derive a 2-10 keV ?ux of 1.5 ± 0.025 × 10?12 and 1.5 ± 0.020 × 10?12 erg cm?2 s?1 from the XMM-Newton (PN) and Chandra data respectively, suggesting that the nucleus presents no variability. However, as the Chandra and XMM-Newton observations are separated by a small interval of about 3 weeks, we have also checked whether other X-ray missions have obtained in the past observations of our object. ROSAT (PSPC) has observed IRAS200511117 in the second semester of 1990 during the ROSAT-All-Sky-Survey (exposure time 411s). The count rate of 0.07 ± 0.01 (0.1-2.4 keV) translates to an absorbed ?ux of 8.4 ± 1.2 × 10?13 erg cm?2 s?1 in the 0.3-2 keV band (using the best-?t PN model). This is consistent with the observed XMM-Newton and Chandra ?ux in the same energy band (? 1×10?12 erg cm?2 s?1 ), within ? 1.3σ.


The X-ray spectra

The spectra are grouped, using the ftool grppha task to give a minimum of 20 (15) counts per bin for XMM-Newton (Chandra ) to ensure that Gaussian statistics apply. The quoted errors to the best ?tting spectral parameters correspond to the 90 % con?dence level for one interesting parameter. In order to assess the signi?cance of new parameters added

–6– to a model we have adopted the 95 % con?dence level, using the F-test for additional terms. We discard data below 0.3 and above 8 keV due to the low response of the ACIS-S, PN and MOS cameras. We ?t the data using the XSPEC v11.2 software package. The spectral ?ts are presented separately for the Chandra and the XMM-Newton data. a) The XMM-Newton spectral ?ts. We ?rst ?t the PN data using a single power-law model absorbed by two columns: one ?xed to the Galactic (NH ≈ 7×1020 Dickey & Lockman 1990) and one intrinsic which is left free to vary. We ?nd that this model provides a relatively poor ?t (χ2 = 268.7/190) to the data. The power-law has the ’canonical’ slope, Γ = 1.92+0.08 , ?0.07 while the 90 % upper limit of the intrinsic column is < 1 × 1020 cm?2 . The addition of a narrow line (σ < 0.01 keV i.e. smaller than the CCD’s spectral resolution at these energies) at 6.4 keV (rest-frame) results in a better ?t. We ?nd ?χ2 = 10.3 for one additional parameter (the normalization of the Gaussian line) which is statistically signi?cant at the > 99 % con?dence level. The equivalent width of the Fe line is 360+174 eV ?170 consistent with that predicted for unobscured AGN (e.g. Page et al. 2004) with comparable X-ray luminosity. The spectral results are presented in table 1. In Fig. 3 (upper panel) we plot the model ?t to the data together with the data to model ratio. Inspection of the residuals suggests the possibility that some additional lines are present: e.g. Fe at 6.96 keV, Ca at 3.9 keV, Si at 1.9 keV (rest-frame). However, only the ?rst line (Fe) is detected at over the 95 per cent con?dence level. The resulting equivalent width is 371+263 eV. ?206 The presence of residuals at low energies prompted us to test for the presence of thermal emission. The inclusion of a Raymond-Smith spectrum (abundance ?xed at Z=0.3) results in a signi?cantly better ?t χ2 ≈ 233.3/186. The temperature of this component (kT = 0.20+0.06 ?0.02 keV) is consistent with the properties of hot gas emission in nearby star-forming galaxies (e.g. Stevens et al. 2003). Its luminosity is L0.3?8keV ? 2 × 1041 erg s?1 . The MOS data are ?tted with the normalizations untied between the MOS1 and MOS2 detectors. The single power-law model gives a good ?t (χ2 = 128.5/121) with a photon index Γ = 2.0+0.11 and an intrinsic column density of 5+2 × 1020 cm?2 . The low e?ective area of the ?0.09 ?1 MOS detectors at high energies, hampers us from placing any constraints on the properties of the Fe lines above 6 keV. The addition of an Fe line results in the reduction of the χ2 by only 0.1. Moreover, the inclusion of a Raymond-Smith component is not statistically signi?cant. Finally, a joint ?t to the PN and MOS data (with the normalizations between the 3 detectors untied) yields Γ = 1.96+0.06, NH = 2+1 × 1020 cm?2 (χ2 = 381.9/313). The ?0.06 ?1 normalizations between the 2 MOS instruments agree within 5% while those between MOS and PN within 20 %. The inclusion of the two Fe lines and the Raymond-Smith component is statistically signi?cant yielding Γ = 1.96+0.08 , NH = 3+2 × 1020 cm?2 (χ2 = 347.9/307). ?1 ?0.06 b) The Chandra spectral ?ts. A single power-law ?t to the data gives Γ = 1.79 ± 0.04

–7– with a negligible intrinsic column density of 0.1 × 1020 cm?2 (χ2 = 290.5/202). The above ν values are in reasonable agreement with those derived from the PN. The addition of an Fe line at 6.4 keV reduces the χ2 by 6.9 which is statistically signi?cant at the ≈ 97 % con?dence level. The equivalent width of the line is 250 ± 155 eV, comparable to the value found from the model ?tting of the PN data. The Chandra spectrum is plotted in Fig. 3 (lower panel) together with the data to model ratio. Finally, the addition of a Raymond-Smith component results in the improvement of the ?t (χ2 ≈ 246.3/199). The temperature of the Raymond-Smith component is 0.22 ± 0.03 keV in good agreement with XMM-Newton while the power-law photon index is ?atter (1.67 ± 0.05). The reduction of the χ2 , when the thermal component is added, may suggest the presence of a compact nuclear star-forming region. Alternatively, it is possible that many photo-ionization line residuals at soft energies are reduced with the inclusion of the above component.


Optical Observations

Optical spectroscopic observations were made with the 1.3 m telescope at Skinakas Observatory (Crete, Greece) on 2002 June 21. The f/7.7 Ritchey-Cretien telescope was equipped with a 1024 × 1024 SITe chip plus a 651 lines mm?1 grating, giving a dispersion of ? 3.3 ?/pix. We used a 2′′ slit which corresponds to a physical size of 1.4 kpc at the A redshift of our object. The spectra span the 4300 ? 7400 ? range, at a resolution of ? 7.0 A ?FWHM. The total integration time was 1.5 hrs. A The optical spectrum of the source is shown in Fig. 4. It is similar to the spectrum presented by Moran et al. (1996). We detect strong Hα, [N II], [S II] and [O III] and much weaker Hβ (narrow) and [O I] lines. Hα has a broad component with a width of ? 3800 km/sec. Our measurements of the galaxy emission line ?ux ratios are as follows: [O III]/Hβ(narrow)=1.1, [O I]/Hα(narrow)=0.019, Hα(narrow)/Hβ(narrow)=2.65, Hα(broad)/Hβ(narrow) =3.69, [NII]/Hα(narrow)=0.59, and [SII]/Hα(narrow)=0.33. The ratios for the bright lines are slightly smaller (by a factor of ? 1.5 ? 2.5) than the respective values listed in Table 3 of Moran et al. (1996). These di?erences are not highly signi?cant, specially if one considers the fact that di?erent ratio values can be obtained if the seeing and/or extraction apertures di?er since in this case di?erent amounts of the host galaxy are included in the aperture. Furthermore, for the fainter lines (Hβ and [O I]) our measurements are quite uncertain because of the poor quality of the data (the overall signal-to-noise of the optical spectrum is ? 5). Despite these small di?erences, the position of the source on the standard emission line diagnostic diagrams (e.g. Veilleux et al. 1995) con?rms that this object lies between the HII region and AGN loci.

–8– From the ratio between Hα(narrow) and Hβ, we calculate a reddening of E(B ? V) = ?0.08 and E(B ? V) = 0.002 for an AGN and an HII region intrinsic continuum respectively. These correspond to an equivalent HI column density of 4 × 1020 cm?2 and 1 × 1019 cm?2 , assuming Galactic gas-to-dust ratio (Bohlin et al 1978). As the reddening mentioned above refers to the sum of the Galactic and intrinsic extinction, this result agrees well with the result of no intrinsic absorption as derived from the model ?tting to the EPIC PN X-ray spectrum.


The spectral energy distribution (SED)

The availability of simultaneous UV (OM) and X-ray (EPIC-PN) observations by XMMNewton gives us the opportunity to investigate the UV/X-ray energy distribution of the source. For the OM data, we ?rst estimated the mean count rate of the individual images (as formed by summing the counts within a 16′′ diameter aperture centered on the nucleus). We have not corrected for the contribution of the underlying galaxy, which increases towards larger wavelengths (reaching ? 30 % in the B ?lter). We transformed the average count rates to magnitudes using the appropriate ’Zeropoint magnitude’ value for each ?lter (as listed in the XMM-Newton users manual). For the reddening correction we assumed no intrinsic absorption, and adopted the Galactic extinction value, AV ≈ 0.4, of Schlegel et al. (1998). Using the Aλ versus λ relationship of Cardelli et al. (1989) for RV = 3.1, we then found Aλ at λ = 4400, 2900, and 2150 ? (i.e. the wavelengths at which the response of the B, UVW1, A and UVW2 ?lters peaks). The UV/X-ray energy distribution is shown in Fig. 5, plotted as νfν versus ν. For the X-ray data we used the best ?tting power law model to the XMM-Newton EPIC-PN spectrum (the long dashed lines represent power law models with slopes equal to the best ?tting slope ±1σ con?dence limit values). In the UV band, the ratio νfU V W 2 /νfU V W 1 is comparable with the ratio of the respective frequencies. This result implies that νfnu ∝ ν, in agreement with the trend shown by the mean energy distribution of radio-quiet AGN in the same energy band (e.g. Elvis et al. 1994). Using the data shown in Fig. 5, we ?nd that the monochromatic X-ray (2 keV) to UV (2500 ?) luminosity ratio for IRAS20051-1117 is A αox = 1.42. This is consistent with the average value of ? 1.6 for radio-quiet AGN (Stocke et al. 1991). The OM, B band measurement indicates that the SED rises towards longer wavelengths. This trend is caused by the fact the host galaxy’s underlying emission in this band is quite stronger than the emission in the UV wavelengths. A quasi-simultaneous ?ux measurement at longer wavelengths is also possible based on the optical spectrum of the source. Since

–9– this spectrum was taken only ? 2.5 months after the XMM-Newton observation we used it in order to estimate a “V” band measurement. To that aim, we computed the average ?ux in the 5400 ? 5600 ? band (observer’s frame), which is free of lines, and we dereddened A it adopting AV ≈ 0.4, as before. Interestingly, although the optical spectrum was taken using a 2′′ wide slit (i.e. signi?cantly smaller than the aperture size that we use for the OM photometry), the V band ?ux that we measure is larger than that in the B band. This result gives further support to the idea that the SED rises towards longer wavelengths. This trend is con?rmed when we consider the near and far infrared measurements of the source. For the J, H, and K bands we used the 2MASS measurements (in a aperture of size 14′′ × 14′′ ). For the far-infrared band we used the IRAS measurements at 25, 60, and 100 microns, from the IRAS faint source catalogue. Although the near-infrared and UV ?ux measurements are taken from apertures which have almost identical areas, the strong rise from optical to near-infrared wavelengths shown in Fig. 5 shows that the energy release in the near-infrared band is signi?cantly larger than that released in the UV band. In IRAS200511117, it is the near-infrared/optical which rises above its UV continuum, and not the other way around, as it is observed in most galaxies with a strong active nucleus. Apart from the strong contribution of the galaxy stellar population in the near-infrared bands, the strong far infrared emission is indicative of the presence of a signi?cant star formation rate (SFR). For example, using the relation between logarithm of SFR and logarithm of galaxy luminosity at 100 microns of Misiriotis et al. (2004), we ?nd an overall SFR of ? 32 M⊙ yr?1 . This is typical of bright IRAS galaxies, but much smaller than SFR in starburst galaxies.



In this work, we present the results from X-ray and optical observations of IRAS200511117. The Chandra and XMM-Newton OM images reveal the presense of a strong, UV and X-ray bright nuclear source, which is un-resolved in both cases. The FWHM of the X-ray source is ? 1′′ , which corresponds to a region of size ? 0.7 kpc at the distance of the object. The X-ray spectrum of the nucleus is very similar to the typical AGN spectra: a power-law model ?tting to the EPIC-PN spectrum shows the canonical spectral slope of Γ ? 1.9, and reveals the presence of an iron line at 6.4 keV. The equivalent width of the line is consistent with that of unobscured AGN of comparable luminosity (e.g. Page et al. 2004). We also detect evidence for the presence of ionized material in the vicinity of the nucleus, as indicated by the presence in the spectrum of a line at 6.96 keV which we interpret as emission from ionized iron. Thermal emission with a low temperature (0.2 keV) is present

– 10 – in both the XMM-Newton and the Chandra spectrum. The presence of a strong, point-like nuclear UV and X-ray source, with an X-ray spectrum typical of AGN, shows conclusively that the intense X-ray emission of IRAS20051-1117 is produced by a Seyfert-like nucleus in the center of this galaxy. This is further supported by the fact that the UV/X-ray energy spectral distribution of this object is very similar to the SEDs of AGN in the same energy band. In particular, the “X-ray loudness” of this object, αox ≈ 1.4, is consistent with the average X-ray/UV luminosity ratio found for radio-quiet AGNs. However, optical observations that were performed only 2.5 months after the XMMNewton observations of IRAS20051-1117, reveal an optical spectrum very similar to the spectrum presented by Moran et al. (1996). The emission-line ?ux ratios places this galaxy on the boundary between regions ordinarily populated by HII and Seyfert galaxies. Although there are signs of Seyfert activity as well (such as the presence of a weak, broad component of the Hα line), the optical spectrum is dominated by characteristics of HII galaxies. Moran et al. (1996) have suggested that “obscuration” e?ects may be responsible for the optical spectra of “composite” galaxies. However, both the XMM-Newton and Chandra observations of IRAS20051-1117 show no sign of any intrinsic absorption in this galaxy. There is a possibility that the X-ray nucleus is totally obscured (Compton-thick) in which case we are viewing the re?ected component in the backside of the torus. The lack of variability between the XMM-Newton and the Chandra epochs (as well as the ROSAT epoch) could in principle favor such an interpretation. Nevertheless, the moderate equivalent width of the Fe line, combined with the steep X-ray spectrum (see e.g. Matt et al. 1996) argue against the re?ection component scenario. The detection of a strong nuclear UV source and of a broad Hα in the low signal-to-noise optical spectrum further support the hypothesis that we are viewing directly the Seyfert nucleus. Ward et al. (1988) have noted the presence of a tight correlation between the broad Hα and the hard X-ray (2-10 keV) luminosity in unobscured AGN. Our object has an Hα luminosity of 7 × 1040 erg s?1 (Moran et al. 1996) which translates to a predicted 2-10 keV X-ray luminosity of 4 × 1042 erg s?1 , in excellent agreement with the Chandra and XMM-Newton observations, further suggesting that the Broad Line Region is not obscured in our object. One possibility that could explain the optical spectral properties of IRAS20051-1117 is that it hosts a non-standard broad line region. For some reason, much less gas in the central source of this object is illuminated by the ionizing continuum, than in a typical AGN. Or perhaps, the broad line region may even be absent in this source. A third possibility though, and perhaps a more realistic one, is that the AGN optical signature is not evident in this source because of the presence of a starburst component (Moran et al., 1996) and because

– 11 – it is partially diluted by the presence of the strong optical continuum of the host galaxy. IRAS20051-1117 is a luminous spiral galaxy, as its optical/near-infrared excess emission in the overall SED implies (Fig. 5). Its total K-band magnitude is 11.28 (2MASS survey) which translates to an absolute magnitude of MK = ?24.5. Using an average colour of R?K = 2.36, appropriate for spiral galaxies of morphological type 0 ≤ T ≤ 6 (de Jong, 1996), we ?nd MR = ?22.14. Severgnini et al. (2003) estimate that the optical signature of X-ray unabsorbed AGN with X-ray luminosity up to ? 1043 erg s?1 (the case of IRAS20051-1117), may be hidden if they are hosted by a galaxy with MR ≤ ?22. In fact, their calculations indicate that only Hα will show clearly the appearence of the central active nucleus, exactly like the case with IRAS20051-1117, as only Hα shows clear evidence for a broad component. Finally, we do not detect any signi?cant variations in both the Chandra and XMMNewton light curves. X-ray variability has become one of the de?ning characteristics of AGN the last years. However, the lack of detection of signi?cant variations is not surprising, given the short duration of the X-ray light curves. For example, the XMM-Newton EPICPN light curve is less than 10 ksec. For a ? 1043 erg/s source, we expect to measure an 2 “excess variance”, σnxs (i.e. the variance of a light curve normalized by its mean squared after correcting for the experimental noise) of ? 0.01 in light curves as long as ? 1 day (e.g. Nandra 2 et al., 1997). If σnxs increases proportional to the length of the light curve, then we expect 2 σnxs ? 0.0015 in the case of the present IRAS20051-1117 light curves. However, due to the low count rate, even in the combined EPIC PN and MOS light curve, the uncertainty on the 2 estimation of σnxs due to the experimental Poisson noise (found using equation 11 of Vaughan et al., 2003) is twice as large as the expected “signal” that we want to detect. Clearly, a longer X-ray light curve is needed in order to detect signi?cant, short term variations in IRAS20051-1117. More surprising is the lack of “long term” variations, when we compare the observed X-ray ?ux during the XMM-Newton Chandra and ROSAT observations, which are separated by 3 weeks and 12 years, respectively. Only monitoring X-ray observations over a period of months/years could allow us to investigate the variability behavior of this source.



We present Chandra and XMM-Newton observations of IRAS20051-1117 one of the ’composite’ galaxies in the Moran et al. (1996) sample of galaxies. The Chandra data show that the X-ray emission comes from a nuclear point-like source with a luminosity of L(2 ? 10keV) ? 4 × 1042 erg s?1 . This coincides with a bright, UV nucleus as revealed by the UV imaging performed with the OM on-board XMM-Newton . The X-ray spectrum

– 12 – (XMM-Newton and Chandra ) is represented by a power-law spectrum with a steep photon index Γ ? 1.7?1.9 and a thermal component with a temperature of ? 0.2 keV absorbed by a negligible intrinsic column density < 3 × 1020 cm?2 . An Fe line at 6.4 keV is also detected in both the XMM-Newton and Chandra data with an equivalent width of ? 300 eV. The above give away the presence of an active nucleus. There is no variability between the Chandra and the XMM-Newton ?ux which are separated by a small period of about 3 weeks. Puzzlingly, there is no observed variability in the soft X-ray ?ux between XMM-Newton and Chandra and the ROSAT observation which are separated by a period of more than 12 years. The marked lack of variability could suggest the presence of a highly obscured (Compton-thick) AGN. However, this possibility is probably ruled out by the moderate equivalent width of the Fe line, the steep X-ray spectrum observed and the ratio of the hard X-ray to the Hα luminosity which are typical of unobscured AGN. The nuclear optical spectrum (using a 2′′ slit which corresponds to a ≈ 1.5 kpc region at the source) obtained 2.5 months after the XMM-Newton observation, presents a weak broad Hα line. Nevertheless, the optical spectrum is dominated by a strong star-forming component which outshines the AGN signatures. The weakness of the AGN features could be attributed to the dilution of the nuclear AGN emission by the star-forming component and the strong host galaxy optical emission. IRAS20051-1117 presents many similarities with the luminous X-ray galaxies which have been detected in deep X-ray surveys. Although these are clearly associated with AGN having high X-ray luminosities, their optical spectra show no AGN signatures. The present observations help us to shed light on the properties of such objects and to understand why these fail to reveal strong AGN signatures in the optical band. This work demonstrates in agreement with earlier work (Georgantopoulos et al. 2003, Severgnini et al. 2003) that heavy obscuration may not always be responsible for the discrepancy observed between the X-ray and optical classi?cation. This work has been supported by the NASA grant G01-2120X. Support is also ackowledged by the grant ’X-ray Astrophysics with ESA’s mission XMM’ in the framework of the programme ’Excellence in Research’ jointly funded by the the European Union and the Greek Ministry of Development. Skinakas Observatory is a collaborative project of the University of Crete, the Foundation for Research and Tecnology-Hellas, and the Max-Planck-Institut f¨ r Extraterrestrische Physik. This research has made use of the NASA/IPAC Extragalactic u Database (NED) which is operated by the Jet Propulsion Laboratory, California Institute of Technology, under contract with the National Aeronautics and Space Administration.

– 13 – REFERENCES Alexander, D.M. et al. 2003, AJ, 126, 539 Barger, A.J., Cowie, L.L., Mushotzky, R.F., Richards, E.A., 2001, AJ, 121, 662 Bohlin, R.C., Savage, B. D., Drake, J.F., 1978, ApJ, 224, 132 Boyle, B.J., McMahon, R.G., Wilkes, B.J., Elvis, M., 1995, MNRAS, 276, 315 Cardelli, J.A., Clayton, G.C., Mathis, J.S., 1989, ApJ, 345, 245 Comastri, A., et al., ApJ, 571, 771 de Jong, R.S., 1996, A&A, 313, 377 Dickey, J.M., Lockman, F.J., 1990, ARA&A, 28, 215 Elvis, M., et al., 1994, ApJS, 95, 1 Georgantopoulos, I., Zezas, A., Ward, M.J., 2003, ApJ, 584, 129 Green, P.J. et al. 2004, ApJS, 150, 43 Gri?ths, R.E., Georgantopoulos, I., Boyle, B. J., Stewart, G.C., Shanks, T., della Ceca, R., 1995, MNRAS, 275, 77 Matt, G., et al. 1996, 281, L69 McHardy, I.M., et al., 1998, MNRAS, 295, 641 Misiriotis A., Papadakis I.E., Kyla?s N.D., Papamastorakis J., 2004, A&A, 417, 39 Moran, E.C., Halpern, J.P., Helfand, D.J., 1996, ApJS, 106, 341 Moran, E.C., Lehnert, M.D., Helfand, D.J., 1999, ApJ, 526, 649 Moran, E.C., Filippenko, A.V., Chornock, R., 2002, ApJ, 579, L71 Mushotzky, R.F., Cowie, L.L., Barger, A.J., Arnaud, K. A. 2000, Nature, 404, 459 Nandra, K., George, I.M., Mushotzky, R.F., Turner, T.J., Yaqoob, T. 1997, ApJ, 476, 70 Page, K. L., O’Brien, P.T., Reeves, J. N., Turner, M.J.L., 2004, MNRAS, 347, 316 Schlegel, D.J., Finkbeiner, D.P., Davis, M., 1998, ApJ, 500, 525 Severgnini, P. et al. 2003, A&A, 406, 483 Stevens, I.R., Read, A.M., Bravo-Guerrero, J., 2003, MNRAS, 343, L47 Stocke, J., et al. 1991, ApJS, 76, 813 Vaughan, S., Edelson, R., Warwick, R.S., Uttley, P., 2003, MNRAS, 345, 1271 Veilleux S., Kim D.-C., Sanders D.B., Mazzarella J.M., Soifer B.T., 1995, ApJS, 98, 171

– 14 – Veron, P., Veron, M.P., Bergeron, J., Zuidervijk, E.J., 1981, A&A, 97, 71 Ward, M. J., Done, C., Fabian, A.C., Tennant, A.F., Shafer, R.A., 1988, ApJ, 324, 767 Watson, M.G., 2001, A&A, 365, L51 Weisskopf, M.C., O’dell, S.L., van Speybroeck, Leon P., 1996, SPIE, 2805, 2 Zezas, A., Georgantopoulos, I., Ward, M.J., 1998, MNRAS, 301, 915

A This preprint was prepared with the AAS L TEX macros v5.2.

– 15 –

Table 1: The spectral ?ts results Γ NH 20 10 cm?2 PN 1.94+0.08 4+3 ?0.10 ?2 MOS 2.00+0.11 5+2 ?0.09 ?1 PN+MOS 1.96+0.08 3+2 ?0.06 ?1 ACIS-S 1.67+0.05 <2 ?0.05

E1 keV 6.4 6.4 6.4

E2 kT keV keV 6.96 0.20+0.06 ?0.02 6.96 0.24+0.06 ?0.06 +0.03 0.22?0.03

χ2 /dof 233.3/186 128.5/121 347.9/307 246.3/199

– 16 –

Fig. 1.— The X-ray contours from the 0.3-8 keV Chandra image, overlayed on the XMMNewton OM image (U ?lter). The line corresponds to 10′′ .

– 17 –

1.2 EPIC-PN Count Rate 0.9








3000 4000 Time (sec)



0.4 Count Rate





10000 Time (sec)



Fig. 2.— Upper panel: XMM-Newton EPIC-PN, MOS-1 and MOS-2, background subtracted, 0.3 ? 8 keV light curves of IRAS20051-1117, grouped in 200 s bins (open spqaures, ?lled and open circles respectively). Time is counted from the start of the PN observation (for clarity reasons the points have been sifted by +50 s on the time axis). Lower panel: Chandra , background subtracted, 0.3 ? 8 keV light curves of IRAS20051-1117, grouped in 1500 s bins. Time is counted from the start of the Chandra observation (for clarity reasons the points have been sifted by +300 s sec on the time axis).

– 18 –

Fig. 3.— The XMM-Newton PN (upper panel) and Chandra (lower panel) spectra plotted together with a model ?t consisting of a power-law plus a 6.4 keV Gaussian line, absorbed by the Galactic and an intrinsic column density. The data to model ratios are given as well.

– 19 –


fλ (erg cm s ? )


-2 -1 -1



0 4500


5500 λ (?)




Fig. 4.— The optical spectrum of IRAS20051-1117 taken in June 2002, from Skinakas observatory. The spectrum, plotted as ?ux per unit wavelength interval, has been shifted to rest frame.

– 20 –



νFν (erg s cm )




























Frequncy (Hz)
Fig. 5.— The rest frame, dereddened continuum energy distribution of IRAS20051-1117. Note that the apertures used to derive ?uxes in the various bands do not have the same size (see text for details).

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