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Temporal Gain Correction


[Hasinger and Snowden1990]

The detector gain (i.e., pulse height as a function of energy) changes slowly due to variations in the gas density, composition, high voltage, pressure, and temperature. The temporal gain variation is corrected by normalizing the event pulse height by a function of the temporal gain G(t) (see Chap. 8).  

In-orbit, temporal variations in the PSPC gain are monitored using an X-ray calibration line (at 1.49keV) provided by the Al K tex2html_wrap_inline16917 source on the PSPC filter wheel (Sect. 3.3.2).  

The actual frequency of the gain calibration measurements, (each taking tex2html_wrap_inline16921 minutes) depends on the mission phase but calibrations are performed at least once per weak. There are small temporal gain variations  of less than 1% within each orbit. Investigations of these variations are under way, the results will be addedto the handbook when they are available.

The effect of the temporal gain correction (applied on top of the gain saturation correction) is demonstrated in Fig. 3.14 for a range of nominal gains. The channel offset is the rough number (position gain corrections are not considered here) of channels added to the PHA channel to produce the PI channel.  

Figure 3.14: The difference between the true and measured pulse height channel. The curves of Fig. 3.13 are now corrected for the variations in absolute gain. The curves are for nominal gains of 90 (top), 100, 110, 120, 130, 140, and 150 (bottom). The deviations from straight lines are caused by corrections for the gain saturation effect [Hasinger and Snowden1990].

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