Our galaxy sample is comprised of 9 edge-on spirals for which we already possess deep images
in the H
emission-line (
Å). These galaxies were originally
selected on the basis of their appearing nearby (apparent diameter 5-10') and having
inclinations within a few degrees of edge-on (R96). We added to this NGC 891 which has been
extensively studied by one of us (Rand 1998; Rand et al. 1990) and, as already indicated,
represents the archetypal or prototypal "chimney galaxy''. It is important to emphasize that
our main sample has not been chosen on the basis of either high emission-line
brightness or enhanced far-infrared (FIR) luminosity. It is expected then to preclude any
bias towards active or starburst galaxies, making our results far-reaching in the sense that
they will apply to typical spiral disks. We use both the FIR luminosity and the ratio of
FIR-to-blue luminosities to check the level of recent star-formation in our sample. Both
quantities are known to assume high values in systems displaying starburst activity (Heckman
et al. 1990; Soifer et al. 1997; Alton et al. 1998b). High Resolution IRAS maps (HiRes) at
60 and
m were obtained on request from the Infrared Processing and Analysis Center
at Caltech (IPAC). These data, in conjunction with optical photometry from the RC3 (de
Vaucouleurs et al. 1991), allowed us to infer mean values of 4.6 109
and 1.1 for the FIR luminosity and
-to-LB ratio respectively
(Table 1). These quantities correspond much better to the properties of nearby,
optically-selected IRAS galaxies (
and 0.6 respectively) rather
than to starburst disks (
and
respectively), and confirms that
our sample consists chiefly of quiescent rather than starburst galaxy types (Soifer et al.
1987; Heckman et al. 1990). We can be less sure that NGC 891 complies with the original
selection criteria. It is indeed one of the nearest examples of a large edge-on disk but an
extensive history of observation indicates that it possesses a fairly active halo which is
probably fed by a disk harbouring fairly vigorous star-formation. The FIR properties of NGC
891 indicate somewhat enhanced levels of recent star-formation over "normal'' disks but
Table 1 shows that this galaxy is much better classified as a quiescent rather than
a starburst system.
Galaxy |
Other Designation | Type | R.A. | Dec. | D |
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(J2000) | (J2000) | (Mpc) | (mag) | (1010![]() |
||||
NGC 891 | UGC 01831 | Sb | 02 22 33.0 | +42 20 56 | 9.5 | 10.5 | 1.4 | 3.2 |
UGC 4278 | IC 2233 | Sd | 08 13 58.8 | +45 44 36 | 10.6 | 12.9 | 0.014 | 0.23 |
NGC 4013 | UGC 06963 | Sbc | 11 58 31.1 | +43 56 50 | 17.0 | 12.2 | 0.47 | 1.6 |
NGC 4217 | UGC 07282 | Sb | 12 15 50.7 | +47 05 37 | 17.0 | 12.0 | 0.80 | 2.4 |
NGC 4302 | UGC 07418 | Sc | 12 21 42.3 | +14 35 52 | 16.8 | 12.4 | 0.22 | 0.93 |
NGC 4762 | UGC 08016 | SO | 12 52 56.3 | +11 13 48 | 16.8 | 11.1 | <0.025 | <0.033 |
NGC 5023 | UGC 08286 | Scd | 13 12 12.0 | +44 02 20 | 6 | 12.9 | 0.0049 | 0.25 |
NGC 5746 | UGC 09499 | Sb | 14 44 56.4 | +01 57 16 | 29.4 | 11.2 | 0.66 | 0.29 |
NGC 5907 | UGC 09801 | Sc | 15 15 54.0 | +56 19 45 | 14.9 | 11.1 | 0.76 | 1.25 |
UGC 10288 | - | Sc | 16 14 25.0 | -00 12 25 | 31.5 | 13.8 | 0.26 | 1.13 |
Galaxy |
Telescope | Observing date | Exposure | Seeing FWHM |
(min) | (arcsec) | |||
NGC 891 | Skinakas 1.3 m | October 1996 | 80 | 1.4 |
UGC 4278 | INT 2.5 m | December 1995 | 10 | 2.5 |
NGC 4013 | Skinakas 1.3 m | June 1995 | 140 | 1.2 |
NGC 4217 | JKT 1.0 m | April 1999 | 90 | 1.2 |
NGC 4302 | INT 2.5 m | April 1991 | 17 | 1.3 |
NGC 4762 | JKT 1.0 m | March 1994 | 90 | 1.6 |
NGC 5023 | JKT 1.0 m | April 1993 | 60 | 2.0 |
NGC 5746 | INT 2.5 m | June 1990 | 8.3 | 1.8 |
NGC 5907 | Skinakas 1.3 m | May 1997 | 30 | 1.8 |
UGC 10288 | JKT 1.0 m | April 1999 | 90 | 1.2 |
In order to carry out a rigorous search for extraplanar extinction features we required deep, optical images for our sample. For a few of the galaxies in Table 1 (NGC 891, NGC 4013, NGC 5907), we were already in possession of deep B, V and R images taken with the 1.3-m telescope at Skinakas Observatory, Greece (Xilouris et al. 1999). For the remainder, we carried out B-band imaging at the Kitt Peak 0.6-m telescope during April 1998 but bad weather prevented us from obtained images with sufficient signal. To complete coverage of the sample we accessed data from the Isaac Newton Group (ING) archive at Cambridge. Table 2 summarizes the sources and important properties of the B-band data. Since our sample was not observed under constant seeing conditions using an identical instrumental set-up we will examine, at a later stage, the effect that varied observing conditions might have on our sensitivity to extraplanar dust.
The archive data were reduced in the standard manner using the STARLINK software package CCDPACK to perform debiasing, flatfielding and sky subtraction etc. We also removed the effects of cosmic rays by aligning and median stacking multiple exposures of the same object. It was not necessary to photometrically calibrate any of the images. Neither the recognition of dust chimneys nor the calculation of optical depth for such features relies on the absolute brightness of the galaxy but solely on the relative difference in brightness between attenuated regions and adjacent, unextinguished regions.
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