The results of these comparisons performed on the corrected measurements are:
The internal comparison between the repeated measurements of the same galaxies reveals a mean error of 0008 (the same order of magnitude as the total mean internal error of 00093), in agreement with the analysis of the error sources in the previous section.
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Most of the galaxies in our sample were previously measured, in particular by the Lick group (Davies et al.1987 - hereafter LICK, and Faber et al.1989 - hereafter 7Sam). Recently the full Lick/IDS (Image Dissector Scanner) database of indices for 381 galaxies and 38 globulars was published by Trager et al.(1998 - hereafter Lick98). This dataset should be regarded as the last version of the Lick/IDS line-strength index system, and we re-scaled all the HYPERCAT data to it.
The estimate of the external errors, and of the corrections to the Lick98 system is done iteratively, and globally for all the HYPERCAT datasets, by inter-comparing these datasets. The comparisons are performed on the aperture-corrected data. For present datasets, the significant intersections are with the LICK dataset (Davies et al.1987) and with Lick98.
After these comparisons, for 59 galaxies in common with other datasets a difference of Mg2(our) - Mg2( HYPERCAT) = 00180002 was found. Such difference between flux-calibrated measurements, like ours, and the Lick/IDS data which are normalized via quartz flat field are indeed not surprising. Analysing the details of the pair-comparisons, we adopted a correction of 0.019 for all datasets except Mar93 (0.025) and Mar95 (0.016).
The parameters of our datasets are given in Table 3 (available in electronic form only).
We summarize in Table 2 the final comparisons between the LICK and Lick98 datasets, our datasets and the HYPERCAT homogenized data. The residual zero-points are negligible, and the mean differences give estimates of the internal errors (on the diagonal of the table are comparisons between consecutive observations; on the other positions are comparisons between different observing runs), and external errors (last three columns). The comparison between our fully corrected measurements and HYPERCAT values is presented in Figs. 1 and 2 (the distributions of residuals with the two major datasets of Table 2 have basically the same form).
Note that the mean residuals between the fully corrected data and the HYPERCAT values are not strictly null, but simply statistically unsignificant. This is because the homogenisation process (Golev & Prugniel 1998) rests on pair-wise comparison and iteratively determines zero-points and weights for all the datasets in HYPERCAT. Such process is not stable and thus is hand-controlled at each iteration (this control consists in under-relaxing the corrections to damp the oscillations).
We also searched for correlations between the mean difference of our Mg2-index measurements and any of these datasets (as some non-linearity in the whole acquisition chain could produce). We did not find any significant effect.
In Table 4 we present the mean corrected value of Mg2 rescaled to the Lick system and the corresponding rms error for the 87 galaxies in the sample. In the electronic version of the table more information for each galaxy is provided, e.g. the flow-smoothed velocity used for aperture correction (defined as the velocity of the cosmologic flow associated with the galaxy).
Figure 1: Comparison between our fully corrected Mg2-index measurements and HYPERCAT values for 59 galaxies in common |
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