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6. A case study, a crowded PSPC field

Our algorithm yields very satisfactory results for long PSPC sequences (exposure time tex2html_wrap_inline1311 ksec), since in these cases the observations have high probability to be contaminated by particle and/or solar background. Figure 5 (click here) shows the results of the screening procedure on RP 200020, a sequence pointed at the Hyades open cluster with 40412 s exposure time. The sources have been detected using the Wavelet transform algorithm developed by Damiani et al. (1997a). In this run, our algorithm has rejected tex2html_wrap_inline1313 s (8% of the total exposure time). In the figure, we show a scatter plot of tex2html_wrap_inline1315 (SNR of the sources in the screened observation) versus tex2html_wrap_inline1319 (SNR of the sources in the unscreened observation). The detection threshold (tex2html_wrap_inline1323) is marked by the dashed linesgif, while the solid line divides the plot in the region where tex2html_wrap_inline1329 (upper left) and the region where tex2html_wrap_inline1331 (lower right). We have displayed only the sources with 4<SNR<6, to stress the behavior of the screening algorithm on faint sources. In the plot, we have 15 sources with tex2html_wrap_inline1329, of which 8 were not detected in the unscreened data but were detected in the screened data when running the detection algorithm at the 4.35 tex2html_wrap_inline1337 threshold. These sources are in the upper left shaded area. On the other hand, we have 9 sources with tex2html_wrap_inline1331, of which none moved below the detection threshold after the screening (lower right shaded area). We therefore have 8 new detections in the screened data set. Since there are 6 sources detected with 4.35<SNR<6 in the unscreened sequence, we have obtained a gain of more than 100% in the number of faint detected sources by running our screening algorithm. In addition, we have an average SNR gain of tex2html_wrap_inline1345% for the matched sources with 4.35<SNR<6 (2.5% considering all sources with SNR>4.35). This is in agreement with the results of previous tests on simulated data sets which showed the advantages of tailoring the algorithm for the case of a faint template source. We note that at the chosen threshold, the algorithm is expected to detect one spurious source per field (Damiani et al. 1997b), and therefore essentially all the new sources in the screened sequence should be real. To provide more confidence on this result we have tried to find counterparts for the 8 new sources using the SIMBAD database and the MPE ROSAT PSPC Catalogue, finding counterparts in 5 cases and none in the remaining.

  figure384
Figure 5: tex2html_wrap_inline1351 scatter plot of RP 200020. Symbols represent off axis angles of displayed sources in arcmin (legend in the plot). Arrows mark upper limits for sources detected only, for instance, in the screened observation and not detected in the unscreened one or vice versa. Dashed lines correspond to the typical detection threshold used in the Wavelet transform detection algorithm of Damiani et al. (1997a,b), while the solid line marks tex2html_wrap_inline1353. Sources moved above detection threshold after the screening process lie in the upper-left dashed area with a dotted line pattern (8 new sources), while sources moved below the detection threshold would be in lower left dashed area (none in this case). New sources are not concentrated at large off-axis angles, where the PSPC PSF is not circular simmetric, but they are at a wide range of off-axis angles

We have verified that for short PSPC exposures (tex2html_wrap_inline1355 ksec), our algorithm tends to reject less than tex2html_wrap_inline1357% of the total exposure time, in agreement with the expectations. In these cases, the average SNR gain is very small, and the average number of gained sources is negligible.


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