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Point Source Sensitivity


The point source sensitivity for an observation is determined by the minimum number of source counts needed to satisfy particular statistical criteria. For example, source existence might require a signal to noise ratio of 5 in order to avoid spurious detections due to statistical fluctuations. If the observation goal is to measure the x-ray flux from a specific object, then the appropriate signal to noise requirement might be 3.

The signal to noise ratio is given by:


where tex2html_wrap_inline2760 is the number of source counts, and tex2html_wrap_inline2762 is the variance in the total counts (source + background) and is typically given by tex2html_wrap_inline2764

The minimum detectable source count rate corresponding to a particular signal to noise ratio is given by the relationship


where tex2html_wrap_inline2768 denotes the minimum detectable source count rate, tex2html_wrap_inline2770 the total background rate in the detection cell (about tex2html_wrap_inline2772  counts s tex2html_wrap_inline1894 ), t the observation time, and tex2html_wrap_inline2778 the signal to noise ratio (snr) threshold for detection.

This is derived by combining the equations defining the snr and variance, and using the additional relation, counts = rate x time.

As an illustrative example, we show in Figure 11.3 gif the point source sensitivity for tex2html_wrap_inline2778 = 5 versus observing time for a source with a power law spectrum. That is, we assume a point source with a power law spectrum of energy index 0.5 similar to the extragalactic X-ray background. A hydrogen column density of tex2html_wrap_inline2782  cm tex2html_wrap_inline1930 is used. Notice that the sensitivity increases linearly with observing time for short observations where there are virtually no background counts in the detection cell. For observations that are long enough for background to be significant, longer than about tex2html_wrap_inline2786  s, the sensitivity increases only as the square root of the observation time.

In general, the conversion from HRI counts to energy flux depends on the spectrum of the X-ray source. For the power law spectrum characterized by the parameters given above, this conversion is given by: 1 count s tex2html_wrap_inline2788  erg cm tex2html_wrap_inline1930  s tex2html_wrap_inline1894 in the energy band 0.1 to 2.4 keV. The following section discusses the conversion from energy flux to count rate in more detail.

next up previous contents
Next: Expected Count Rates Up: FEASIBILITY: XMA + HRI Previous: General Assumptions

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