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Astron. Astrophys. 339, L73-L76 (1998)
3. Continuum light curves
Altogether, 19 sets of spectra could be secured, of which 14 were
obtained in the course of the monitoring. Most spectra are of very
high quality, some with a continuum S/N ratio exceeding 100 in
component A. Examples of the spectra are presented in Fig. 1; the
range in S/N ratio is bracketed by these example data, with most
spectra looking rather similar to the February 1995 ones. The high
quality of the data enabled us to monitor the monochromatic
continuum fluxes of both components, which has the advantage over
the conventional broad-band magnitudes that it is a brightness measure
uncontaminated by emission lines and their possibly different
variability patterns. However, absolute photometric calibration from
standard stars was usually not possible, and we had to design a method
to compare spectra taken at different epochs. In the following we
motivate and outline this procedure.
![[FIGURE]](img15.gif) |
Fig. 1. Example spectra obtained in the monitoring, showing the region around C IV 1549 for two epochs, in components A and B. The adopted continua are marked by the dotted lines.
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After placing the spectra on a relative flux scale, we measured the
fluxes and equivalent widths of all major emission lines in both
components (Ly , Si IV 1400,
C IV 1549, and C III]
1909). Local continua were estimated by fitting
straight lines to predefined wavebands known to be largely devoid of
emission and absorption lines (cf. examples in Fig. 1). Although
a direct comparison of line strengths between different epochs is not
possible, there is one strong piece of evidence that the lines have
remained essentially constant over the time span observed: The flux
ratio between the same lines in components A and B, independent of the
absolute scale, has stayed at a consistently constant value of
for all lines. This implies either a time delay
of much less than a month (the separation between data points during
the periods of quasi-continuous monitoring), which is highly
improbable, or simply constancy of the line fluxes as such. Adopting
the latter hypothesis, we were then able to recalibrate the spectra by
scaling them to equal emission line fluxes. As reference we used C IV,
a prominent line that is surrounded by clearly identifiable continuum
windows visible also at low spectral resolution.
For each pair of spectra we computed a scale factor so that the
C IV flux of component A assumed an arbitrary but constant value, and
applied this factor to both spectra. The average continuum values in
the interval , thus at
Å, were then determined for A and B. This
estimate of the QSOs brightness is independent of external flux
standards and of photometric conditions, and we were thus able to
incorporate also narrow slit observations by the same method. Note
that the relative flux calibration based on standard stars was not
even strictly needed, although it helped in removing the
instrumentally caused curvature from the spectra. The resulting light
curves are depicted in Fig. 2. The error bars in this plot
contain both the continuum uncertainties due to photon shot noise and
the error of the line flux rescaling factor. The zeropoint for both
components is arbitrarily set at the continuum magnitude of A in May
1993, which constitutes the brightest point.
![[FIGURE]](img20.gif) |
Fig. 2. Monochromatic continuum light curves of both components, taken at Å. The zero point is arbitrary, but the same for both panels. Error bars in the upper panel are generally smaller than the symbol size.
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Although the light curve is certainly not well-sampled, some
features are very cleary discernible. The strong decline in component
A between 1993 and 1995, spanning almost a magnitude, is well mirrored
in B, except for the inflection between Nov 1994 and Feb 1995 which
occurs only in B. This feature alone is already very suggestive that B
leads the variability, as one expects from the observed lens
configuration (cf. R98). From early 1996 on, the sampling improved due
to the beginning of regular monitoring, and it became apparent that
the object shows also significant variability on relatively short time
scales.
© European Southern Observatory (ESO) 1998
Online publication: October 22, 1998
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