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Results and Data Products
The best-fit model for each flight detector was used to predict quantum
efficiency as a function of energy. For historical reasons, our fits of
the model to the data (both for the absolute response of the reference
detectors, and the relative response of flight detectors) made use of standard
(Henke, 1993) mass-absorbtion coefficients. It should be noted, however,
that the predicted flight detector efficiency curves incorporate
our measurements of the absorption edge structure near the nitrogen, oxygen
and silicon edges (see section 4.6.4).
As an example, the best-fit quantum efficiency for ACIS detector S2
(the most efficient ACIS FI detector at all energies) is shown in Figure
4.91. The lower panel of the figure
shows estimated 90% confidence envelope on the relative error in the model
quantum efficiency; these error limits are discussed in detail in the next
section.
The adopted quantum efficiency models for the two BI devices are shown
in Figures 4.93 and 4.94.
Figure 4.91: Best-estimates for ACIS
S2 (Front Illuminated) Detector Quantum Efficiency Model and 90% Confidence
Envelope. See text for interpretation of the error envelope.
The best-fit quantum efficiency models for all FI detectors are shown
in Figure 4.92. The quantum efficiency
of the back-illuminated detector S3 is shown in Figure 4.94
Figure 4.92: Best-fit model quantum efficiency for all
ACIS FI Detectors
 |
Figure 4.93: Adopted ACIS S1 (Back-illuminated) Detector
Quantum Efficiency Model
 |
Figure 4.94: Adopted ACIS S3 (Back-illuminated) Detector
Quantum Efficiency Model
 |
The quantum efficiency of each ACIS flight detector will be made available
as an ASCII table file. It is intended that these files be available from
the MIT ACIS web page at
http://acis.mit.edu.
The files can also be found on the MIT CSR ACIS calibration database in
the directory
/ohno/di/database/rsp/release.



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Please address comments and questions to Dr. John Nousek ( nousek@astro.psu.edu
)