A&A 484, 341-345 (2008)
DOI: 10.1051/0004-6361:20077444

The core flux of the brightest 10 $\mu $m galaxies in the southern sky[*],[*]
(Research Note)

D. Raban1 - B. Heijligers1 - H. Röttgering1 - K. Meisenheimer2 - W. Jaffe1 - H. U. Käufl3 - T. Henning2


1 - Leiden Observatory, Leiden University, PB 9513, Leiden, 2300 RA, The Netherlands
2 - Max-Planck-Institut für Astronomie, Königstuhl 17, 69117 Heidelberg, Germany
3 - ESO, Karl-Schwarzschild-Str. 2, 85748 Garching bei Muenchen, Germany

Received 9 March 2007 / Accepted 26 March 2008

Abstract
Aims. Near diffraction-limited images have been taken at 8.9, 11.9, and 12.9 $\mu $m for the brightest extragalactic sources in the southern sky, in order to optimally plan N-band observations with MIDI (MID-infrared Interferometric instrument) at the VLTI.
Methods. We have assembled a sample of 21 objects consisting of all the AGNs observable from Paranal observatory, Chile, plus three non-AGN objects, with an estimated N-band flux greater than 400 mJy. We used the TIMMI2 Mid Infrared instrument mounted on the ESO's 3.6 m telescope to obtain near diffraction-limited images in order to establish the unresolved core flux within <0.5 arscsec.
Results. Positions and core total fluxes were obtained for all sources in our sample and compared with similar investigations in the literature. We find that 15 AGN and the nuclear starburst in NGC 253 exhibit an unresolved core flux <300 mJy at 11.9 $\mu $m, making them promising targets for MIDI at the VLTI. For extended sources, near diffraction-limited images are presented and discussed.

Key words: techniques: photometric - galaxies: active - galaxies: nuclei - galaxies: Seyfert - infrared: galaxies

1 Introduction

Since the operation of MIDI at the VLTI began in 2004, astronomy has entered a new era where it is now possible to reach a resolution of a few milliarcseconds at infrared wavelengths, about 15 times the resolution of the largest single-dish telescopes. MIDI operates in the N-band (8-13 $\mu $m) and therefore it is ideal for observing heated dust expected in AGNs and starburst galaxies. Although it is most commonly used in observing galactic objects like circumstellar disks (Leinert et al. 2004) and dust shells around evolved stars (Ohnaka et al. 2005), MIDI has been successfully used to observe extragalactic objects. The main limitation of MIDI in this context is its limiting flux of $\sim$400 mJy, so only bright objects can be observed currently. So far, MIDI has been used to observe dusty tori in AGNs, objects which are central to the AGN unification model, and which have proven too small to be resolved by a single dish telescope. With its superior resolution, the presence of a torus-like structure has been established in the galaxy NGC 1068 (Jaffe et al. 2004) by using only two baseline observations, and additional MIDI observations with extensive coverage of up to 21 baselines have measured the geometrical properties of the torus in the Circinus galaxy (Tristram et al. 2007) and NGC 1068 (Raban et al., submitted). A resolved dust structure was also detected in the core of Centaurus A (Meisenheimer et al. 2007). Apart from active galactic nuclei, the only extragalactic objects bright enough for MIDI are starburst galaxies. For such objects, MIDI can be used to measure the size and geometry of the nuclear star-forming region.

Here, we have assembled a list of the brightest extragalactic objects at 10 $\mu $m, and observed them at 8.9, 11.9 and 12.9 $\mu $m with the TIMMI2 instrument, mounted on the 3.6 m telescope in La Silla, Chile. Our goal here is to give the basic information needed in order to plan VLTI observation of cores of galaxies. Positions and core fluxes were determined for all sources, and for those sources which were resolved, we present and discuss images at 8.9, 11.9 and 12.9 $\mu $m.

The layout of the paper is as follows: in Sect. 2 we describe how the observed sources were selected; the observations and data reduction are discussed in Sects. 3 and 4; images are presented in Sect. 5 along with a brief description of each object and additional reference information

  
2 Sample selection

The target list consists of all AGN's observable from Cerro Paranal ($\delta<22$) and have an estimated total N-band flux density brighter than N=5 or SN=400 mJy, which is the limiting magnitude for observations with MIDI, estimated from previous N-band measurements available in the literature. This list of 21 objects (without NGC 1068) was taken from the catalogue of Seyfert galaxies by Lipovetsky et al. (1988) to which we added additional sources from the compilations of Granato et al. (1997) and Maiolino et al. (1995), plus the IR luminous galaxy M 83, the starburst galaxy NGC 253 and the famous quasar 3C 273. See Table 1 for a complete list.

Table 1: Observation list and fluxes for all objects.

  
3 Observations

The mid-infrared observations were carried out with the TIMMI2 instrument on the ESO 3.6 m telescope on La Silla, Chile, on the nights of 6 and 7 of August 2001 and 8 to 10 February 2002. TIMMI2 is a mid-infrared imager and spectrograph operating in the M (5 $\mu $m), N (10 $\mu $m) and Q (20 $\mu $m) atmospheric bandpasses. The camera is equipped with a 320 $\times$ 240 pixel Si:As array and can operate at a scale of 0.2 or 0.3 arcsec/pixel. We used the 0.2 arcsec/pixel scale resulting in a total field-of-view of $64\hbox{$^{\prime\prime}$ }$ $\times$ $48\hbox{$^{\prime\prime}$ }$. For a complete description of the instrument refer to Reimann et al. (2000) and Käufl et al. (2003).

For most of the observations we selected the 1.2 $\mu $m wide 11.9 $\mu $m filter since it offered the best signal to noise ratio for a given integration time. A ratio of flux over noise (per pixel) of about a 200 is achieved by 40 min of integration time for a 400 mJy source. Sources that were significantly brighter were observed for shorter periods of time. Some targets were supplemented with additional images with the the 8.6 $\mu $m filter ( $\Delta\lambda=1.2$ $\mu $m) and the 12.9 $\mu $m filter ( $\Delta\lambda=0.9$ $\mu $m). The complete observation log can be found in Table 1.

Seeing conditions as monitored in the optical were highly variable, ranging between 1 and 1.8 arcsec on August 6 to 0.36 and 0.8 arcsec on August 7, 2001, while the humidity at ground level remained around 5%. During the February 2002 run the seeing was constant at 1 arcsec with a very high humidity at ground level of 80-95%. In order to remove the strongly variable background radiation of the telescope and atmosphere in the mid infrared we used the standard chopping and nodding method. In this mode the secondary mirror chops with a frequency of typically several Hz North-South and the telescope is nodded approximately every 5 min East-West. As all sources turned out to be compact at 10 $\mu $m, the small field chop and nod mode was used, keeping the objects always in the frame, while still avoiding overlapping of the images which might lead to loss of flux. This effectively cuts the field-of-view of the chip in 4 pieces and is therefore only possible for compact targets, such as extended star forming regions. The relatively small throw we used can substract these from the image, leading to an underestimation of the flux. During chopping the detector is continuously read-out with a frequency of about 40 Hz and each 100 image pairs are subtracted, stacked and saved to disk. The result is a series of chopped frames with both a positive and a negative image of the source, with an exposure time of approximately 25 s per frame. Subtracting 2 frames from different nod positions results in 2 positive and 2 negative acquisitions of the object. We used a of 20 arcsec North-South and a nod of 30 arcsec East-West (except for the observations of M 83 where these values were 25 and 30 arcsec respectively), allowing for both the chopped as well as the nodded positions to fall onto the detector, while at the same time preventing any overlap of the positive and negative images.

Due to technical problems with the autoguider there was a slow position drift during the integrations. This was taken into account during data reduction.

  
4 Reduction

Standard reduction techniques were used to convert a set of raw frames into a final, photometrically calibrated image of the source. Flat field correction was not applied since for all ground-based mid-IR instruments no possibility of a reliable flatfield correction exists up to now (Starck et al. 1999), and since the chopping and nodding method used to eliminate the thermal background results in a relatively flat images. For our data cosmic rays removal is not required since the number of background photons is large, making the cosmic ray's contribution undetectable. Bad pixels were detected using the statistical variation of each pixel, extrapolated and excluded from the measurements. Three different modes for referencing and co-adding were implemented to accommodate different SNR levels. For all these modes the image peak was determined by fitting a Gaussian of appropriate size to the central airy disk:

Since the transmissivity of the atmosphere is highly variable in the observed wavelengths, absolute calibration is challenging. The system is photometrically calibrated using bright stars of known flux that have been observed every two hours. Care was taken that the stars are observed at similar altitudes to the science objects. For the photometry measurement a distinction is made between objects where the nucleus is a mere point source and objects displaying extended emission. For point sources a $1.6\hbox{$^{\prime\prime}$ }$ aperture flux was taken, covering the central airy disk out to the first minimum. For extended objects the peak value was used since the PSF is well sampled with $0.2\hbox{$^{\prime\prime}$ }$ per pixel. Using the peak value minimizes contamination from extended components. For these sources the growth curve of the source and the PSF are also presented in order to make clear which part of the flux comes from an unresolved source. The peak flux corresponds to an aperture of 1.2 $\hbox{$^{\prime\prime}$ }$. An exception is NGC 7582, for which the flux was measured with a $2.6\hbox{$^{\prime\prime}$ }$ aperture. In order to improve the visual appearance all images have also been deconvolved, using a simple but robust, CLEAN method, where a PSF taken from a nearby reference star is iteratively subtracted from the peak position and replaced with a Gaussian with a similar width. Flux errors are dominated by the calibration errors from the reference stars measured by estimating the fluctuations of the transmissivity of the sky by comparing the fluxes of the same objects (stars or AGNs) close in time. Accordingly, the photometric error is about 15% for all sources.

  
5 Results

Core flux measurements and core positions for each source are presented in Table 1. Figures A.1 to A.8 show high resolution contour images of eight objects out of the 21 objects observed, omitting those sources for which more recent images are available and images of unresolved sources. A brief discussion of each source is presented, along with references for other similar or complementary data. All sources show an unresolved core with little or no extended emission, with the exception of NGC 253, NGC 7582, NGC 1365, and M 83, which show considerable extended emission.

NGC 253.
Figure A.1. This nearby starburst galaxy shows complex extended emission in all observed wavelengths: 8.6, 11.9 and 12.9 $\mu $m. All images show two sources, the bright source seems to be resolved. The extended emission shows an elongation of 3'' to the north east. An additional peak is seen clearly in the 8.6 $\mu $m image, and to a lesser extent in the 11.9 $\mu $m image, and corresponds to ``peak 3'' that Kalas & Wynn-Williams (1994) identify at 3.28 $\mu $m and is most likely to be PAH emission. The 12.9 $\mu $m image, shows the structure boarded by the two peaks reported by Boeker et al. (1998) as well as other authors, and is very similar to the NeII map of these authors and the NeII maps of Keto et al. (1999). It is most likely to be dominated by a combination of NeII emission and 12.7 $\mu $m PAH emission (Boeker et al. 1998; Förster Schreiber et al. 2003). Since the 11.9 filter is centered on 11.66 $\mu $m with a FWHM of 1.16 $\mu $m it is likely that the 11.9 $\mu $m extended emission also includes 11.3 $\mu $m PAH emission. Galliano et al. (2005) show 11.9 $\mu $m deconvolved images and identify six sources, as opposed to four in our 11.9 $\mu $m image Comparing the two images, sources M2 and M3 of Galliano et al. (2005) coincide with our second brightest peak, and sources M5 and M6 with the two peaks to the North-East. The flux measured by Galliano et al. (2005) for the main peak (5000 $\pm$ 1000 mJy) is a factor of two higher than the flux measured in this work. This discrepancy can be attributed to the 2'' aperture used by Galliano et al. (2005) as opposed to out method of measuring the peak value (see Sect. 4) Identifying out second peak with M2+M3 our flux (1150 mJy) is 50% higher than the combined flux of M2 and M3.

NGC 1365.
Figure A.2. A face-on spiral galaxy with a prominent bar. Our 11.9 $\mu $m image shows an unresolved nucleus and two point sources to the north east, identified by Galliano et al. (2005) as M5 and M6. This structure is surrounded by an arm like faint extended emission. In addition, the deconvolved image shows slight point like emission from sources M7 and M4 of Galliano et al. (2005). The authors identify their M4, M5 and M6 sources with radio counterparts of Saikia et al. (1994), and conclude that these sources are embedded young massive star clusters. Flux measurements of the nucleus are in excellent agreement with Galliano et al. (2005), but are higher than those of Siebenmorgen et al. (2004) who measured a flux of 400 mJy at 8.5 $\mu $m and 460 mJy at 10.4 $\mu $m. This discrepancy can be explained by the multi-source structure of NGC 1365, causing flux measurements very sensitive to telescope positioning. The weak extended emission to the South West of the nucleus also appears as two point sources in the 11.9 and 10.4 $\mu $m deconvolved maps of Galliano et al. (2005) and is most likely not an artifact.

IRAS 05189-2524.
Observations of this Seyfert 2 galaxy at $11.9~\mu$m show a completely unresolved core with no deviations from the PSF larger then $1\sigma$. An unresolved core is also reported by Siebenmorgen et al. (2004) with 8.6, 10.4 and 11.9 $\mu $m flux densities of 420, 420 and 570 mJy, respectively, and by Soifer et al. (2000), who present a 12.5 $\mu $m image and 12.5 24.5 $\mu $m fluxes.

NGC 2377.
For this object we give an upper limit for the flux of 60 mJy.

MCG 5-23-16.
For this S0 galaxy hosting a Seyfert 1.9 nucleus we have an unresolved core with a flux of 646 mJy at 11.9 $\mu $m.

Mrk 1239.
Figure A.3. Observations of this highly polarised narrow-line Seyfert 1 galaxy at 11.9 $\mu $m shows central source unresolved. The 11.9 $\mu $m flux is in agreement with Maiolino et al. (1995).

NGC 3256.
Our image (not presented here) of this IR-luminous merger system shows an unresolved core, In contrast to Siebenmorgen et al. (2004) who present a resolved, yet featureless image, taken with shorter exposure time. The difference may be explained by a change in seeing between the calibrator, from which the PSF is determined, and NGC 3256.

NGC 3281.
For this Seyfert 2 galaxy we measure 625 mJy for 11.9 $\mu $m, which is similar to the N-band flux found at Krabbe et al. (2001) 580 $\pm$ 30 mJy, measured with a 2.2 m telescope, and therefore a diffraction limit 1.6 times that of our observation. A 18'' $\times$ 20'' 10.5 $\mu $m image of NGC 3281 dominated by a point source and marginal evidence for an extended emission component is also presented by Krabbe et al. (2001).

NGC 3758.
(Mkn 739) For this double-nuclei Seyfert I/starburst galaxy a low flux of <60 mJy is measured.

NGC 3783.
NGC 3783 is a nearly face-on SBa galaxy with a very bright, highly variable, Seyfert 1 nucleus. The image shows an unresolved point source.

3C 273.
The image of this well known quasar shows an unresolved core at 11.9 $\mu $m. The measured 11.9 $\mu $m flux is in agreement with the N-band flux of Sitko et al. (1982) but 100 mJy higher than the flux quoted in Gorjian et al. (2004).

NGC 4594.
``Sombrero Galaxy''. For this object the measured 11.9 $\mu $m flux, <60 mJy, is in agreement with the results found at Maiolino et al. (1995) and Gorjian et al. (2004).

MCG-3-34-6.
The low flux measured here, <60 mJy at 11.9 $\mu $m is much smaller than the 440 mJy flux measured by Maiolino et al. (1995) at 10.4 $\mu $m, with a 5.4'' aperture. The origin of the discrepancy are unclear since this object has not been studied before apart from the single measurement of Maiolino et al. (1995) mentioned above, and so it is possible that the N-band emission is variable. Our image shows an unresolved point source and therefore it is unlikely that extended emission is responsible for the discrepancy.

NGC 5128.
Figure A.4. Centaurus A, the closest active radio galaxy. The 11.9 $\mu $m image shows an unresolved central core, with extended emission at 10% level. The 8.6 $\mu $m image shows an unresolved core. For comparison, see Siebenmorgen et al. (2004) for a 10.4 $\mu $m image showing an unresolved core of less than 0.5''.

M 83.
Figure A.5. This near, face-on barred spiral galaxy shows mostly extended emission surrounding a faint central object. The extended emission is dominated by PAHs which account for the majority if the MIR luminosity (Vogler et al. 2005). The $11.9~\mu$m flux measured, 232 mJy, is identical with the $11.9~\mu$m flux measured by Siebenmorgen et al. (2004). Our images, however, show a clear, although faint, central source, while Siebenmorgen et al. (2004) report only fuzzy extended emission. The LW3 filter (12-18 $\mu $m) of Vogler et al. (2005) show the emission clearly tracing the spiral arms of M 83, which is not seen in our image.

ESO 445-G50.
For this Seyfert I galaxy we measure 352 mJy at 11.9 $\mu $m. A 10.4 $\mu $m flux of 640 mJy can be found at Siebenmorgen et al. (2004).

Mrk 463.
The image of this double-nuclei Seyfert 2 galaxy shows an unresolved core at 11.9 $\mu $m, measuring 338 mJy.

Circinus.
Figure A.6. Observations of this nearby spiral were made at 11.9 $\mu $m and 8.6 $\mu $m. The seeing at for the 11.9 $\mu $m point was bad, so no statement can be made whether the central peak is resolved or not. The 8.6 $\mu $m does show a slightly resolved background component yet whether this is a disk or circum-nuclear emission (reported by Krabbe et al. 2001 with a radius of $\approx$1'' is not clear. The image presented here is very similar to the one presented by Siebenmorgen et al. (2004). Recent high resolution 8.74 and 18.33 $\mu $m images and flux measurements are also presented by Packham et al. (2005), which also find a higher 8.74 $\mu $m flux, 5.5-8.4 Jy, for a range of apertures from 1'' to 5''.

NGC 5506.
Figure A.7. For this edge-one irregular Seyfert 1 (S1i) galaxy, we show here the first high resolution images at 8.6 and 11. 9 $\mu $m. The 8.6 $\mu $m image shows an unresolved core while extended emission to the north-east is seen in the $11.9~\mu$m image. The 11.9 $\mu $m flux measured, 908 mJy, is similar to the Siebenmorgen et al. (2004) measurement of 1060 mJy.

NGC 7469.
For this prototypical Seyfert 1 galaxy we encountered an unknown image quality problem. Soifer et al. (2003) present a high resolution (4'' $\times$ 4'') 12.5 $\mu $m image of the nucleus of NGC 7469, resolving the ring structure around the nucleus and an extended structure in the nucleus itself.

NGC 7582.
NGC 7582 is a classic Seyfert 2 galaxy which, during a period of five months in 1999 showed broad lines characteristic of a Seyfert 1 galaxy, which may indicate the presence of a patchy torus. Aretxaga et al. (1999). 50% of the flux found in extended emission with a peak offset from the center of the extended emission. The extended emission is seen elongated along the South-North direction. The 12.9 $\mu $m image shows two weak sources to the North and to the South of the main peak, also clearly seen in the 12.9 $\mu $m image of Acosta-Pulido et al. (2003). The 11.9 $\mu $m image shows one slightly resolved peak surrounded by extended emission. Flux at 11.9 $\mu $m is very similar to that of Siebenmorgen et al. (2004), although the 11.9 $\mu $m image they present shows considerably less extended emission. Similar extended emission can also be seen in the N1 ($\approx$8-95.5 $\mu $m) image of Acosta-Pulido et al. (2003).

  
6 Conclusion

We presented new high resolution mid-infrared images and fluxes at 8.9, 11.9 and 12.9 $\mu $m for the brightest AGN's observable from Cerro-Paranal. Most sources show an unresolved core, with little or no extended emission. Considerable extended emission has only been detected for NGC 253, NGC 7582 and M 83. For each source, a brief discussion is given along with a comparison with other relevant published data. In general we find our images and fluxes to be in agreement with previous papers.

References

 

  
Online Material

Appendix A: Figures


  \begin{figure}
\par\mbox{\includegraphics[width=6cm,clip]{7444fg1A.ps} \includeg...
...H.eps} }
\phantom{\includegraphics[width=6cm,clip]{7444fg1H.eps} }
\end{figure} Figure A.1: NGC 253 contour and image overlays, Left: raw data. Right: central point deconvolved with CLEAN algorithm sdf. Bottom: growth curve of the core and PSF at 11.9 $\mu $m ( left) and 8.9 $\mu $m ( right).
Open with DEXTER


  \begin{figure}
\par\mbox{\includegraphics[width=8cm,clip]{7444fg2A.ps}\hspace*{1...
...e*{1.5cm}
\phantom{\includegraphics[width=8cm,clip]{7444fg2C.ps} }
\end{figure} Figure A.2: NGC 1365 Contour and image overlays. Left: raw data. Right: central point deconvolved with CLEAN algorithm sdf. Bottom: comparison of X and Y axis crosssection with psf, in normalized counts.
Open with DEXTER


  \begin{figure}
\par\mbox{\includegraphics[width=8cm,clip]{7444fg3A.ps} \includeg...
...e*{4cm}\includegraphics[width=8cm,clip]{7444fg3C.ps}\hspace*{4cm}}
\end{figure} Figure A.3: Mrk 1239 contour and image overlays, see Fig. A.2.
Open with DEXTER


  \begin{figure}
\par\mbox{\includegraphics[width=7cm,clip]{7444fg4A.ps}\hspace*{4...
...4E.ps} \includegraphics[width=7cm,clip]{7444fg4F.ps}\hspace*{4cm}}
\end{figure} Figure A.4: NGC 5128 contour and image overlays, see Fig. A.2.
Open with DEXTER


  \begin{figure}
\par\mbox{\includegraphics[width=8cm,clip]{7444fg5A.ps}\hspace*{2...
...e*{2cm}
\phantom{\includegraphics[width=8cm,clip]{7444fg5C.eps} }
\end{figure} Figure A.5: M 83 contour and image overlays, see Fig. A.2. Bottom: growth curve of core compared with the PSF.
Open with DEXTER


  \begin{figure}
\par\mbox{\includegraphics[width=7cm,clip]{7444fg6A.ps}\hspace*{3...
...ce*{3cm}
\phantom{\includegraphics[width=7cm,clip]{7444fg6E.ps} }
\end{figure} Figure A.6: Circinus contour and image overlays, see Fig. A.2.
Open with DEXTER


  \begin{figure}
\par\mbox{\includegraphics[width=7cm,clip]{7444fg7A.ps}\hspace*{3...
...7E.ps} \includegraphics[width=7cm,clip]{7444fg7F.ps}\hspace*{3cm}}
\end{figure} Figure A.7: NGC 5506 contour and image overlays, see Fig. A.2.
Open with DEXTER


  \begin{figure}
\par\mbox{\includegraphics[width=7cm,clip]{7444fg8A.ps}\hspace*{3...
...g8E.ps}\includegraphics[width=7cm,clip]{7444fg8F.ps}\hspace*{3cm}}
\end{figure} Figure A.8: NGC 7582 contour and image overlays, see Fig. A.2.
Open with DEXTER



Copyright ESO 2008