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To compare measurements of relative quantum efficiency made at MIT CSR and XRCF, we have used the data in Table 4.27 to compute relative QE ratios referenced to device S2. The results are presented in Table 4.29. Similarly, we have compiled relative QE ratios referenced to S2 from telemetry data taken at XRCF (see Table 4.30). The telemetry data was taken using windows near the top and bottom of each device to avoid saturating the telemetry stream. In Table 4.31 we have computed the fractional difference (CSR-XRCF/CSR) between the relative QE measurements made at each site. The relative QE ratios at XRCF for the FI devices are in excellent agreement with the ratios obtained at CSR. This provides additional evidence that spatial variations in efficiency are small in the FI devices and that the absolute efficiencies of these chips are nearly identical at each energy.
The agreement between XRCF and CSR is not as good for the BI devices. At 0.525 keV, both S1 and S3 appear to have been 10-15% more efficient relative to S2 in the XRCF data compared to the CSR data. Smaller discrepancies are also apparent at several other energies. The origin of these discrepancies is not understood. Examinations of the effects of windowing at XRCF and differences in the source spectra at CSR and XRCF have not resolved this issue.
Device | Position | Mean (RMS) Relative Efficiency vs. Energy (keV) | ||||||
0.525 | 0.677 | 1.740 | 2.015 | 4.509 | 5.894 | 8.040 | ||
O | F | Si | P | Ti | Fe55 | Cu | ||
w203c4r | I0 | 0.860 | 0.791 | 0.993 | 0.920 | 0.990 | 0.970 | 0.936 |
(0.031) | (0.031) | (0.043) | (0.040) | (0.043) | (0.044) | (0.044) | ||
w193c2 | I1 | 0.877 | 0.796 | 0.976 | 0.950 | 0.990 | 0.967 | 0.898 |
(0.037) | (0.036) | (0.052) | (0.052) | (0.050) | (0.053) | (0.054) | ||
w158c4r | I2 | 0.906 | 0.834 | 0.987 | 0.964 | 0.991 | 0.965 | 0.905 |
(0.038) | (0.038) | (0.052) | (0.051) | (0.050) | (0.052) | (0.051) | ||
w215c2r | I3 | 0.883 | 0.808 | 0.993 | 0.924 | 0.976 | 0.977 | 0.932 |
(0.032) | (0.031) | (0.040) | (0.038) | (0.038) | (0.040) | (0.041) | ||
w168c4r | S0 | 0.935 | 0.867 | 1.001 | 0.947 | 0.993 | 0.965 | 0.919 |
(0.037) | (0.035) | (0.042) | (0.039) | (0.041) | (0.041) | (0.042) | ||
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 | 0.903 | 0.858 | 1.002 | 0.951 | 0.995 | 0.991 | 1.003 |
(0.032) | (0.036) | (0.045) | (0.043) | (0.043) | (0.045) | (0.048) | ||
w201c3r | S5 | 0.889 | 0.823 | 0.996 | 0.926 | 0.995 | 0.992 | 1.008 |
(0.032) | (0.032) | (0.042) | (0.039) | (0.041) | (0.043) | (0.047) | ||
w140c4r | S1 | 2.985 | 2.589 | 1.030 | 1.431 | 0.930 | 0.718 | 0.524 |
(0.155) | (0.139) | (0.065) | (0.104) | (0.092) | (0.066) | (0.047) | ||
w134c4r | S3 | 2.950 | 2.399 | 1.068 | 1.461 | 1.003 | 0.833 | 0.640 |
(0.139) | (0.168) | (0.060) | (0.085) | (0.064) | (0.058) | (0.052) |
Device | Position | Mean Relative Efficiency vs. Energy (keV) | ||||||||
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 | 0.839 | 0.808 | 0.962 | 0.980 | 0.950 | 0.981 | 0.948 | 0.903 | |
w193c2 | I1 | 0.873 | 0.803 | 0.965 | 0.978 | 0.962 | 0.985 | 0.946 | 0.910 | |
w158c4r | I2 | 0.915 | 0.847 | 0.979 | 0.995 | 0.977 | 0.988 | 0.951 | 0.894 | |
w215c2r | I3 | 0.876 | 0.806 | 0.976 | 0.992 | 0.969 | 0.989 | 0.907 | ||
w168c4r | S0 | 0.687 | 0.908 | 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 | 0.902 | 0.910 | 0.975 | 0.991 | 0.965 | 1.005 | 0.980 | 1.049 |
w201c3r | S5 | 0.625 | 0.880 | 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 | 1.093 | 1.343 | 0.949 | 0.756 | 0.672 |
Device | Position | Frac. Rel. Eff. Diff. vs. Energy (keV) | |||
0.525 | 1.740 | 4.509 | 8.040 | ||
O | Si | Ti | Cu | ||
w203c4r | I0 | +0.021 | +0.013 | +0.009 | +0.035 |
w193c2 | I1 | +0.010 | -0.002 | +0.005 | -0.013 |
w158c4r | I2 | -0.003 | -0.008 | +0.003 | +0.012 |
w215c2r | I3 | +0.020 | +0.001 | -0.013 | +0.027 |
w168c4r | S0 | +0.024 | +0.015 | -0.009 | +0.016 |
w182c4r | S2 | 0.000 | 0.000 | 0.000 | 0.000 |
w457c4 | S4 | +0.007 | +0.011 | -0.010 | -0.046 |
w201c3r | S5 | +0.015 | +0.013 | -0.004 | 0.000 |
FI Mean | +0.013 | +0.006 | -0.003 | +0.004 | |
FI Std Dev. | 0.010 | 0.009 | 0.009 | 0.027 | |
w140c4r | S1 | -0.159 | -0.004 | +0.089 | -0.006 |
w134c4r | S3 | -0.112 | -0.023 | +0.054 | -0.050 |
Mark Bautz