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An image of an on-axis
point source at 6.627 keV is shown in Figure 19.
The structure in the image is due to the quadrant supports and poorly
shaped foils near quadrant boundaries.
The azimuthally averaged point response functions measured at 6.627,
8.837, and 11.046 keV, and their
integrals, the encircled energy functions, are shown
in Figure 20 and Figure 21, respectively.
As in section 3.2, the encircled energy is assumed to be
1.0 in a circle of diameter 105
.
Despite the image asymmetry, the azimuthally averaged point response function
may be adequately represented by the simple function
psf(r) = (a1/r) e-0.5(r/b1)2 + a2 e-r/b2 + a3 e-r/b3
where r is expressed in arc-minutes, and the constants have the
values shown in Table 4.
Table 4:
Point Response Function Model Parameters
| |
| Parameter |
6.6627 keV |
8.837 keV |
11.046 keV |
| a1 |
0.01732 |
TBD |
TBD |
| b1 |
1.835 |
TBD |
TBD |
| a2 |
0.0024 |
TBD |
TBD |
| b2 |
2.659 |
TBD |
TBD |
| a3 |
3.047
 |
TBD |
TBD |
| b3 |
14.559 |
TBD |
TBD |
Figure 17:
SODART on-axis effective area for a single module. The curve
represents the effective area for an ideal x-ray
telescope with the SODART parameters, normalized to measured effective
areas at energies of 6.627, 8.837, and 11.046 keV.
|
Figure 18:
SODART vignetting function measured at three different energies and various
off-axis angles. The solid lines are included to guide the eye only,
and do not represent a functional fit.
|
Figure 19:
On-axis image of a point source at 6.627 keV in FM1. The data were
recorded by an imaging detector similar to LEPC. Adjacent contours
are spaced by a factor of e.
|
Figure 20:
Point Response Function of the SODART MM at three
different energies. The function is estimated from the same data used
to derive the encircled energy function.
|
Figure 21:
Encircled Energy Function of the SODART MM at three different
energies.
|
Next: The High Energy and
Up: The SODART Mirror Modules
Previous: Effective Area and Telescope
Tomas P. Girnius
1999-01-21