Contents of: VI/111/./abstract/YTANIGUC_HYPERGAL.abs

The following document lists the file abstract/YTANIGUC_HYPERGAL.abs from catalogue VI/111.
A plain copy of the file (without headers/trailers) may be downloaded.


Rowan-Robinson et al. (1991) discovered a hyperluminous (L = 10E14 Lsun)
galaxy, IRAS F10214+4724, at redshift of 2.286, among the sources in the IRAS
Faint Source Catalogue. Since this object contains abundant molecular gas
(10E11 Msun: Brown & Vanden Bout 1991; Solomon, Radford, & Downes 1992), it
has been sometimes considered as a possible candidate of proto galaxies (cf.
Elbaz et al. 1992). The optical spectrophotometry has revealed that the
nuclear light is strongly polarized (17%: Jannuzi et al. 1994), suggesting
the presence of hidden AGN. Even though the presence of AGN, IRAS F10214+4724
is one of very important objects to study forming galaxies because of its
high redshift and the unusually abundant molecular gas.
In order to understand the true nature of this kind of hyperluminous infrared
galaxies (HYPERs), we have to measure their star formation activity
 unambiguously. Here we propose to use PAH features observed in near and mid
infrared wavelength regions because they are intimately related to the star
formation activity. The PAH features observed at 3.28, 3.4, 6.2, 7.7, 8.6,
and 11.25 microns are considered as due to transient heating of polycyclic
hydrocarbon molecules by UV photons emitted by OB stars (Leger & Puget
1984). These emission features are indeed not observed in pure AGN like type
1 Seyfert and QSOs because PAHs are destroyed by hard radiation field of AGN
(Aitken & Roche 1985; Voit 1992) while  observed ubiquitously in starburst
galaxies, giving good measures of the star forming activity (Moorwood 1986;
Mouri et al. 1990; Mizutani, Suto, & Maihara 1994). Therefore, we will be
able to understand the star-forming nature of HYPERs. Our targets are (1)
IRAS F10214+4724 (z=2.286: Rowan-Robinson et al. 1991), (2) IRAS F15307+3252
(z=0.925: Cutri et al. 1994), and (3) IRAS 09104+4109 (z=0.442: Kleinmann et
al. 1988). Since the three objects have a wide range of redshift from 0.442
to 2.286, the interesting PAH features are observed at 10 - 15 microns. Thus,
 we need the ISOCAM CVF system to perform this observation.