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5. Notes on individual objects

  A brief discussion is given here on some individual sources.

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IRAS tex2html_wrap_inline2654: This galaxy lies in the sky close to SMC. The field is therefore crowded with SMC foreground stars. This contamination, added to a poor seeing, make it difficult to determine the morphology of the system. However, a central extended object, from which we got the spectrum displayed in Fig. 5 (click here), a tidal tail and two possible companions seem to be associated with IRAS 00199-7426.

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IRAS tex2html_wrap_inline2658: There are two galaxies in the field separated by a distance of 40tex2html_wrap_inline2660 (42 kpc). Surprisingly, the IRAS position is centered on the western object, which is less luminous, in the optical, that the eastern disturbed spiral. Contrary to its companion, the infrared ultraluminous galaxy seems to have a regular spiral morphology. Since IRAS had a limited angular resolution, varying between 1tex2html_wrap_inline2662 and 5tex2html_wrap_inline2662, it is not clear whether in pairs, both galaxies are enhanced in the far infrared (Xu & Sulentic 1991; Surace et al. 1993). In IRAS 09111-1007, the two galaxies (which are indeed at the same distance; the difference in velocity is only 300 km s-1) show strong optical lines. However, compared to the eastern object, the western one is extremely absorbed. Htex2html_wrap_inline2484 is invisible and there is a strong Na absorption line, which indicates a high dust content. Moreover, the radio continuum source associated with this source is stronger than the one associated with the companion (Karoji et al. 1986). Since there is a tight correlation between radio and far infrared fluxes (eg. Wunderlich et al. 1987), we can argue that most of the far infrared luminosity in this system comes from the western component.

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IRAS tex2html_wrap_inline2672: It has two tidal tails, one prominent to the North with a condensation at its tip, and another fainter to the South-East. Both optical and infrared images show a single nucleus. This might be a merger in an advanced stage.

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IRAS tex2html_wrap_inline2674: There is no obvious companion to this elliptical-like galaxy. Faint clumps can be found in the outskirts of the main body. It is likely to be a merger in a final stage.

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IRAS tex2html_wrap_inline2676: The IRAS flux is concentrated on the northern spiral object of this loose interacting pair. The galaxy is highly disturbed. A long tail with bright condensations escapes to the North. An arc structure is seen to the West. Its Seyfert 1 spectrum shows strong iron FeII lines. Two line systems, separated by tex2html_wrap_inline2678, are seen in the tex2html_wrap_inline2680 and [OIII] line profiles. This object will be discussed in more details in a future paper.

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IRAS tex2html_wrap_inline2682: This isolated object has an eccentric nucleus, also seen in the infrared (Murphy et al. 1996), which is an hint for a complete merger classification.

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IRAS tex2html_wrap_inline2684: It has faint tidal tails and a disturbed morphology in the central region, with a bright nucleus surrounded by condensations (similar to HII regions) and absorption features. In the K band however, the dust lanes disappear and only one nucleus shows up. It's luminosity profile follows the classical r1/4 de Vaucouleurs law for ellipticals. This is a case where an elliptical galaxy is being formed after a disk-disk collision. Martin et al. (1989) have shown that this object is an OH megamaser.

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IRAS tex2html_wrap_inline2690: This spectacular object, also known as "the Super-Antennae'' has been discussed in details by Mirabel et al. (1991) and Colina et al. (1991).

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IRAS tex2html_wrap_inline2692: No clear nucleus can be found in either interacting disk. Murphy et al. (1996) have shown that only the EW disk emits in K.

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IRAS tex2html_wrap_inline2696: Two diffuse tails can be seen. The nucleus is clearly elongated to the East in the R band. After a deconvolution by a gaussian PSF, with a Maximum Entropy method, two condensations separated by 2.6tex2html_wrap_inline2660 (4.5 kpc) show up. In the infrared, however there is only a marginal detection at the position of the faintest source.

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IRAS tex2html_wrap_inline2702: With an infrared luminosity of tex2html_wrap_inline2704 tex2html_wrap_inline2058, it is the brightest source of our sample. It appears as a disk-disk collision. The northern disk seems to vanish in the K band.

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IRAS tex2html_wrap_inline2710: This is one of the ambiguous systems in the sample. Two main galaxies are visible, apparently separated by 41 kpc (we do not have a redshift for the eastern object). The IRAS flux is concentrated on the western object. None of the galaxies show clear tidal disturbances. Faint objects can be seen in the vicinity of IRAS 20414-1651/W.

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IRAS tex2html_wrap_inline2714: discussed in details by Johansson (1991). Only one nucleus appears in the R and K bands of this merger.

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IRAS tex2html_wrap_inline2720 (the so-called "South America Galaxy''): Carico et al. (1990) have shown, in the K band image, two nuclei separated by 2tex2html_wrap_inline2660 (3 kpc).

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IRAS tex2html_wrap_inline2726 (the "Bat galaxy''): discussed in details by Bergvall & Johansson (1985) and Johansson & Bergvall (1988). The wings of this object are tidal features, whereas its eyes are the nuclei of the merging galaxies.

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IRAS tex2html_wrap_inline2728: The nucleus seems to be elongated in the optical to the East. After deconvolution with a gaussian, one can infer a nuclei separation of 2.4tex2html_wrap_inline2660 (4.1 kpc). The infrared image shows an elongated nucleus, but does not confirm that it is double.

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IRAS tex2html_wrap_inline2732: Two nuclei are visible but one is at least twice as bright as the other in the optical. In K, the ratio is 10.


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