Astron. Astrophys. 363, 863-868 (2000)
3. Data analysis and results. Temporal analysis
The LECS (0.1-10 keV) and MECS (1.5-10 keV) light curves are shown
in Fig. 1. The source varies as much as a factor
2 on time-scales of a few thousands of
seconds. To search for spectral variability, we have also plotted the
(1.5-4)/(0.1-1.5) LECS hardness ratio, and the (4-10)/(1.5-4) MECS
hardness ratio. Clearly, there is significant spectral variability,
especially in the second part of the observation. To investigate the
energy dependence of this variability, we calculated the Normalized
Excess Variance (NEV; see Nandra et al. 1997) (Fig. 2) for
different energy intervals, using a 128 s binning. The source is
variable at all energies, but the amplitude is the highest around 2
keV.
![[FIGURE]](img9.gif) |
Fig. 1. From top to bottom: LECS light curve and hardness ratio; MECS light curve and hardness ratio; PDS light curve (background subtracted) and PDS/MECS hardness ratio.
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![[FIGURE]](img11.gif) |
Fig. 2. The Normalized Excess Variance for different energy intervals.
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The PDS light curve and the PDS/MECS ratio are also shown in
Fig. 1. The light curve is very variable, the background
subtracted PDS count rates sometimes going down to values consistent
with zero. The light curve is different from those of the LECS and
MECS, suggesting either a strong spectral variability or a significant
contamination by the nearby BL Lac, 2A 1219+305.
© European Southern Observatory (ESO) 2000
Online publication: December 5, 2000
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