As it is apparent from Fig. 1 (click here), there is a clear correlation between the measured relative error and the (S/N-ratio)/Å. Although such a correlation arises naturally, quantitative estimates of errors as a function of (S/N-ratio)/Å are also expected to depend on index values.
We have shown that the use of approximate
formulae for the computation of errors can lead to misleading error
estimates. However, performing appropriate simplifications, it is possible to
derive simple expressions to estimate the absolute index error as a
function of the mean (S/N-ratio)/Å. It can be shown that
where, to simplify, we have defined SN(Å) as
(the summation extends over the three bandpasses, i.e. N pixels).
The two constants c1 and c2 are defined as follows
being ,
and
the
bandpass widths.
Equations (41 (click here)) and (45 (click here))
can be easily employed to predict the required (S/N-ratio)/Å to achieve a
fixed index error. In Fig. 5 (click here) we show the predictions
of these expressions for some particular indices compared with the actual
error measurements (from Eqs. (33 (click here))
and (37 (click here))) in a star sample. It is interesting to note that
the absolute error of molecular indices does not depend, in a first
approximation, on the absolute index value, although the contrary is true for
the atomic indices. This is the reason why a larger scatter is apparent in
panel (a), where in Eq. (41 (click here)) has been
replaced by its corresponding arithmetic mean in the sample. Numerical values
for c1, c2 and c3, which obviously depend on the considered index,
are given in Table 1.
Figure 6: Absolute atomic (panel a)) and molecular (panel b)) line-strength
errors measured in the sample of 40 stars from
the Lick library as a function of the mean (S/N-ratio)/ Å.
The predictions of
Eqs. (41 (click here)) and (45 (click here)) are
plotted as dashed lines
Following the same procedure with the D4000 index:
where SN(Å)b and SN(Å)r,
the mean (S/N-ratio)/Å in the blue and red band
respectively, will attain, in general, different values (given the large
wavelength coverage of the break). In this case, the relative D4000
error does not depend on the absolute D4000 value.