All Tables
- Table 1:
Log of the observations. R gives the average spectral
resolution as measured from the data. The resolution varies by 10%
from one spectrum to the next. The seeing is the one recorded by the
observatory DIMM monitor, and not the effective spatial resolution
obtained from the data cube.
- Table 2:
Fluxes for the strong emission lines in units of
10-16 erg s-1 cm-2 corrected for Galactic extinction. The
magnitudes are given in AB units. The first three rows correspond
to different aperture sizes. For the WR and SN region the
radial apertures are 2
defined to include all the flux from
the regions seen in the H
image. Below the first three rows
the fluxes are extracted from the images in a square
aperture of
spaxels equivalent to 4 arcsec2 around the
coordinates in Col. 1. The magnitudes are calculated from
the spectra extracted within this aperture. Note that the
properties vary with the chosen aperture; especially the equivalent
widths show differences as described in Sect. 3.4.
The oxygen abundance and N/O abundance ratio in the two
last columns are discussed in Sect. 3.8. The
uncertainties for line fluxes and magnitudes are
10%,
<4% for the H
and H
EW, 0.12 mag for the
reddening, and 0.14 dex for the oxygen abundance calibration. The
uncertainty of the N/O ratio is 0.2 dex. The last row gives the
mean of the individual regions, and the uncertainty is
the standard deviation.
- Table 3:
Table for derived quantities for the different regions. The
last row gives the mean and standard deviation for all the
regions. Column 2 is the SFR derived from the observed
H
flux, and Col. 3 corrects the SFR for the extinction given
in Table 2. Column 4 gives the best fit age. The
mass (Col. 5) is determined from population modelling. The mass to
light ratio (Col. 6) uses the luminosity LB derived from the
B magnitude relative to the AB magnitude for the sun
.
Column 7 lists the specific SFR per Gyr
normalised to the mass after correction for the host extinction, and
Col. 8 lists the luminosity specific SFR, both derived after
correcting for intrinsic extinction.