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Ultraviolet sensitivity of the WFC: the ``UV leak''

 

Some of the available WFC filters have a secondary transmission band in the far-ultraviolet. Although these are much weaker than the primary XUV bands, problems may arise when observing objects that have a particularly strong far-UV component in their spectrum. The count rate detected by the WFC will then be an unresolved mixture of XUV and far-UV photons. In severe cases the scientific return of the observation may be compromised. Observers should ensure that their selected targets do not fall into this category. For any target the severity of the potential problem can be assessed by referring to Table 12.1 gif . This lists predicted count rates for each filter from an tex2html_wrap_inline3184 blackbody source at temperatures of 10000, 20000 and 30000 K. The expected far-UV count rate from a target can then be estimated by scaling the tex2html_wrap_inline3184 count rate for the appropriate temperature to the actual tex2html_wrap_inline3168 value (i.e., by multiplying the value given in Table 12.1 gif by tex2html_wrap_inline3190 ). Note that the UV leak is largest for the S2 filter; for the other filters the UV leak is unlikely to be a problem except for the brightest stars.

 

Temp (K) 4 Count rate in each filter (counts s tex2html_wrap_inline1894 )
S1 S2 P1 P2
C/Lexan/B Be/Lexan Al/Lexan Sn/Al
10000 tex2html_wrap_inline3196 tex2html_wrap_inline3198 tex2html_wrap_inline3200 tex2html_wrap_inline3202
20000 tex2html_wrap_inline3204 0.74 tex2html_wrap_inline3206 tex2html_wrap_inline3208
30000 tex2html_wrap_inline3210 2.1 tex2html_wrap_inline3212 tex2html_wrap_inline3214
Table: 12.1   Predicted far-UV count rate for a blackbody source with tex2html_wrap_inline3184


next up previous contents
Next: Variability studies with the Up: FEASIBILITY: THE WIDE FIELD Previous: Comparison with the EXOSAT

Michael Arida
Tue Jun 11 16:18:41 EDT 1996