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Comparison Between MIT and XRCF (Phase I) Measurements of Relative Quantum Efficiency

To compare measurements of relative quantum efficiency made at MIT's Center for Space Research (CSR) and Marshall Spaceflight Center's X-ray Calibration Facility (XRCF), we have used the data in Table 4.54 to compute relative QE ratios referenced to device S2. The results are presented in Table 4.58. Similarly, we have compiled relative QE ratios referenced to S2 from telemetry data taken at XRCF (see Table 4.59). The telemetry data was taken using windows near the top and bottom of each device to avoid saturating the telemetry stream. The pileup correction factors applied to the XRCF count rates are presented in Table 4.60.
 
 
Table 4.58: Spatially Averaged Relative Detection Efficiency at CSR--Referenced to S2. In each box the mean is given as the top entry; the RMS variation is given in parentheses below it.
 
Flight Position Mean (RMS) Relative Efficiency vs. Energy (keV)
Device   0.525 0.677 1.740 2.015 4.509 5.894 8.040
    O F Si P Ti Fe55 Cu
w203c4r I0 0.858 0.790 0.979 0.930 0.990 0.970 0.898
    (0.055) (0.049) (0.071) (0.066) (0.072) (0.074) (0.090)
w193c2 I1 0.878 0.798 0.977 0.949 0.991 0.969 0.907
    (0.058) (0.053) (0.073) (0.069) (0.075) (0.077) (0.087)
w158c4r I2 0.906 0.836 0.983 0.966 0.993 0.965 0.906
    (0.055) (0.051) (0.070) (0.067) (0.071) (0.073) (0.084)
w215c2r I3 0.882 0.809 0.980 0.936 0.991 0.972 0.894
    (0.056) (0.049) (0.074) (0.069) (0.076) (0.079) (0.092)
w168c4r S0 0.939 0.868 0.987 0.960 0.992 0.965 0.881
    (0.058) (0.053) (0.074) (0.070) (0.074) (0.076) (0.091)
w182c4r S2 1.000 1.000 1.000 1.000 1.000 1.000 1.000
    (0.000) (0.000) (0.000) (0.000) (0.000) (0.000) (0.000)
w457c4 S4 0.901 0.853 0.988 0.966 0.995 0.991 0.963
    (0.051) (0.052) (0.063) (0.060) (0.064) (0.068) (0.091)
w201c3r S5 0.886 0.817 0.984 0.939 0.996 0.992 0.967
    (0.051) (0.047) (0.067) (0.061) (0.068) (0.072) (0.095)
w140c4r S1 3.078 2.606 1.033 1.439 0.921 0.715 0.522
    (0.207) (0.159) (0.074) (0.110) (0.093) (0.066) (0.053)
w134c4r S3 2.989 2.417 1.082 1.489 1.004 0.835 0.640
    (0.170) (0.187) (0.084) (0.116) (0.082) (0.072) (0.068)
Table 4.59: Spatially Averaged Relative Detection Efficiency from XRCF Telemetry--Referenced to S2
 
Flight Position Mean Relative Efficiency vs. Energy (keV)
Device   0.277 0.525 0.705 1.487 1.740 2.166 4.509 6.399 8.040
    C O Fe L Al Si Nb L Ti Fe K Cu
w203c4r I0   0.842 0.810 0.962 0.982 0.942 0.981 0.948 0.903
w193c2 I1   0.868 0.805 0.965 0.979 0.954 0.985 0.946 0.910
w158c4r I2   0.909 0.849 0.979 0.996 0.969 0.988 0.951 0.894
w215c2r I3   0.865 0.807 0.976 0.994 0.961 0.989   0.907
w168c4r S0 0.687 0.912 0.873 0.979 0.986 0.964 1.002 0.953 0.904
w182c4r S2 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
w457c4 S4 0.625 0.897 0.910 0.975 0.991 0.965 1.005 0.980 $ 1.049^\ast$
w201c3r S5 0.625 0.876 0.828 0.966 0.983 0.966 0.999 0.972 1.008
w140c4r S1 36.619 3.460 3.022 1.071 1.034 1.287 0.847 0.617 0.527
w134c4r S3 35.679 3.280 3.033 1.115 1.092 1.342 0.949 0.755 0.671
$^{\ast}$ The XRCF bias for this data point is peculiar.

 
Table 4.60: Pileup Correction Factors Applied to Count Rates from XRCF Telemetry
 
Flight Position Pileup Correction vs. Energy (keV)
Device   0.277 0.525 0.705 1.487 1.740 2.166 4.509 6.399 8.040
    C O Fe L Al Si Nb L Ti Fe K Cu
w203c4r I0   1.001 1.007 1.049 1.007 1.020 1.017 1.021 1.119
w193c2 I1   1.001 1.007 1.049 1.007 1.020 1.017 1.021 1.117
w158c4r I2   1.001 1.007 1.050 1.008 1.021 1.009 1.015 1.116
w215c2r I3   1.001 1.007 1.050 1.008 1.021 1.017   1.116
w168c4r S0 1.000 1.001 1.002 1.050 1.008 1.021 1.018 1.028 1.139
w182c4r S2 1.000 1.001 1.007 1.051 1.008 1.022 1.013 1.020 1.140
w457c4 S4 1.000 1.001 1.003 1.050 1.008 1.021 1.011 1.029 1.164
w201c3r S5 1.000 1.001 1.002 1.049 1.008 1.021 1.018 1.029 1.157
w140c4r S1 1.001 1.004 1.007 1.044 1.007 1.029 1.019 1.016 1.036
w134c4r S3 1.001 1.003 1.009 1.046 1.008 1.030 1.016 1.018 1.042




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