CXO Project Science:
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1998 Jun 16 22:00 GMT
In preparation for the AXAF stray-light test, conducted during thermal-Vacuum testing at TRW, AXAF Project Science re-evaluated the focal-plane stray-light requirement based on the as-built performance of the AXAF Science Instrument (SI) detectors. The as-built requirements are comparable to or less demanding than the as-designed ones, and retain some practical margin against those in the Observatory CEI Specification.
The following table summarizes the stray-light requirements at the top of the respective focal plane, for the as-built High-Resolution Camera (HRC) and AXAF CCD Imaging Spectrometer (ACIS). A more detailed table appears later in this report and an active Excel spreadsheet (stray-uvis.xls) is available. For reference, the AXAF Observatory Contract End Item (CEI) Specification is approximately log(PST) < -12 for solar XUV, < -10 for solar UV, < -8 for solar visible, and < -7 for bright-earth visible radiation, at the aperture of the detector.
Detector | HRC-I | HRC-S | HRC-I | HRC-S | HRC-I | HRC-S | ACIS-I | ACIS-S | |
Spectral band | xuv | xuv | uv | uv | vis | vis | vis | vis | |
Max solar PST | Log(PST_sun) | -9.0 | -10.4 | -2.1 | -9.0 | -4.5 | -7.5 | -4.6 | -6.0 |
Max earth (10-Mm) PST | Log(PST_earth10) | -4.7 | -6.0 | +0.4 | -6.5 | -2.9 | -6.0 | -3.1 | -4.5 |
The plots show the spectral flux for direct illumination by the following sources:
The plots show the XUV-visible net efficiency of the AXAF Science Instrument (SI) detectors:
The plots show the spectral count rate for direct illumination of AXAF Science Instrument (SI) detectors by the following sources:
The table shows the requirement on the maximum count rate from stray XUV-visible radiation, the band-integrated count rate for direct illumination by the sun and bright earth, and the consequent maximum PST consistent with each SI detector's stray-light requirement. The spectral bands are 100-500 Angstrom for XUV, 500-3000 Angstrom for UV, and 3000-11000 Angtrom for visible. The requirement on the PST is at the top of the focal plane, i.e., just above the optical filter of the respective SI detector.
Detector | HRC-I | HRC-S | HRC-I | HRC-S | HRC-I | HRC-S | ACIS-I | ACIS-S | |
Spectral band | xuv | xuv | uv | uv | vis | vis | vis | vis | |
Max rate | Log(ct s^-1 cm^-2) | -2.0 | -2.0 | -2.0 | -2.0 | -2.0 | -2.0 | +4.7 | +4.7 |
Direct solar rate | Log(ct s^-1 cm^-2) | +7.0 | +8.4 | +0.1 | +7.0 | +2.5 | +5.5 | +9.3 | +10.7 |
Max solar PST | Log(PST_sun) | -9.0 | -10.4 | -2.1 | -9.0 | -4.5 | -7.5 | -4.6 | -6.0 |
Direct earth (10-Mm) rate | Log(ct s^-1 cm^-2) | +2.7 | +4.0 | -2.4 | +4.5 | +0.9 | +4.0 | +7.8 | +9.2 |
Max earth (10-Mm) PST | Log(PST_earth10) | -4.7 | -6.0 | +0.4 | -6.5 | -2.9 | -6.0 | -3.1 | -4.5 |
Direct earth (100-Mm) rate | Log(ct s^-1 cm^-2) | +1.1 | +2.4 | -4.0 | +2.9 | -0.7 | +2.4 | +6.2 | +7.6 |
Max earth (100-Mm) PST | Log(PST_earth100) | -3.1 | -4.4 | +2.0 | -4.9 | -1.3 | -4.4 | -1.5 | -2.9 |
For the HRC, the as-built requirements on the XUV and UV PST are approximately the same as the as-designed ones. The HRC requirements on the visible PST, although not identified originally, are less stringent than those on the UV PST. For the ACIS, the as-built requirements on the visible PST are a couple orders of magnitude less demanding than the as-designed ones, primarily because of better performance of the ACIS optical blocking filters.
The most stringent SI-detector stray-light requirement is for solar illumination of the HRC-S: log(PST) < -10.4 for XUV or < -9.0 for UV, depending upon the uncertain decrease of reflectance into the XUV. For reference, the AXAF Observatory Contract End Item (CEI) Specification is approximately log(PST) < -12 for solar XUV, < -10 for solar UV, < -8 for solar visible, and < -7 for bright-earth visible radiation, at the aperture of the detector.
Note that the as-built HRC-S requirement has an order-of-magnitude negative margin against the Observatory CEI Specification for stray-visible solar radiation. However, satisfying the CEI stray-UV specification ensures satisfying the visible one, and the CEI specifies the value at the detector's aperture rather than at its focal plane. Furthermore, the TRW design provides several orders of magnitude margin agains
The table compares the count rate of each detector for direct solar illumination and for illumination by a test lamp (100 W at 30 cm). A measured count rate (or upper limit) during the lamp test then provides a calculated value (or upper limit) for the point-source transmittance (PST).
Detector | HRC-I | HRC-S | ACIS-I | ACIS-S | |
Spectral band | vis | vis | vis | vis | |
Pixel density | Log(pixels cm^-2) | +6.4 | +6.4 | +5.2 | +5.2 |
Direct solar rate | Log(ct s^-1 cm^-2) | +2.5 | +5.5 | +9.3 | +10.7 |
Direct lamp rate | Log(ct s^-1 cm^-2) | +2.6 | +5.6 | +9.5 | +10.9 |
The following then gives the point-source transmittance (PST) for visible radiation:
log(PST) = log(measured rate) - log(direct rate).
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