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Examples

  1. The expected count rate from a source with a blackbody spectrum (perhaps a neutron star) needs to be estimated. The source has L tex2html_wrap_inline2836  ergs s tex2html_wrap_inline1894 in the ROSAT energy band (0.1 to 2.4 keV), and is at a distance of 2 kpc with tex2html_wrap_inline2840  cm tex2html_wrap_inline1930 (log( tex2html_wrap_inline2844 ). The assumed temperature is equivalent to 0.1 keV. The unabsorbed flux for this source is tex2html_wrap_inline2846  ergs cm tex2html_wrap_inline1930  s tex2html_wrap_inline1894 , or in units of tex2html_wrap_inline2420 the flux is tex2html_wrap_inline2854 . From the Table 11.5 gif or Figure 11.7 gif the appropriate ECF is tex2html_wrap_inline2856 , and the expected count rate is tex2html_wrap_inline2858  counts s tex2html_wrap_inline1894 . We estimate that a detection of this source at the tex2html_wrap_inline2406 level will require an observation time of about 4,000 s.
  2. Consider a distant AGN with a power law spectrum of energy slope 0.5 which is at a luminosity distance of 1000 Mpc and is viewed through an absorption column of tex2html_wrap_inline2782  cm tex2html_wrap_inline1930 (log( tex2html_wrap_inline2868 ). The AGN luminosity in the ROSAT band is L tex2html_wrap_inline2870  ergs s tex2html_wrap_inline1894 . We want to determine how long an observation is required for a tex2html_wrap_inline2874 detection. The unabsorbed flux is tex2html_wrap_inline2876  ergs cm tex2html_wrap_inline1930  s tex2html_wrap_inline1894 . The ECF for this spectral model is taken from Table 11.3 gif or Figure 11.5 gif, it is tex2html_wrap_inline2882 , which gives a count rate tex2html_wrap_inline2884  counts s tex2html_wrap_inline1894 . Using the sensitivity formula from § 11.2 gif, we calculate that the observation time needed to detect this source at the tex2html_wrap_inline2874 level is about 12,600 s.
  3. What is the conversion factor from counts per second to energy flux for a particular spectrum? For example, a Raymond-Smith Plasma with a temperature corresponding to 1 keV and a column of tex2html_wrap_inline2890  cm tex2html_wrap_inline1930 (log( tex2html_wrap_inline2894 ). The ECF for this spectral model is taken from Table 11.4 gif or Figure 11.6 gif, it is tex2html_wrap_inline2896 . That is, a flux of tex2html_wrap_inline2898  ergs cm tex2html_wrap_inline1930  s tex2html_wrap_inline1894 in the ROSAT energy band (0.1 to 2.4 keV) will give a count rate of tex2html_wrap_inline2896  counts s tex2html_wrap_inline1894 in the HRI. Inverting this relationship gives the result that 1 count s tex2html_wrap_inline2908  ergs cm tex2html_wrap_inline1930  s tex2html_wrap_inline1894 . In general the conversion factor from counts per second to energy flux is given by: 1 count s tex2html_wrap_inline2914 /ECF ergs cm tex2html_wrap_inline1930  s tex2html_wrap_inline1894 .

next up previous contents
Next: Spatial Resolution Up: Expected Count Rates Previous: Expected Count Rates

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