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Consistency of Relative
Spatial Variations in Quantum Efficiency
As discussed in section 4.7.1
above, we have measured quantum efficiency (relative to a reference detector)
of each ACIS flight device as a function of position. For purposes of presentation,
we have binned the relative quantum efficiency into 32-by-32-pixel ``superpixels'';
we expect that in typical AXAF observations the celestial image will be
dithered over an area of about this size (
arcsec) on the ACIS focal plane.
Maps showing the spatial uniformity of the relative quantum efficiency
at each measurment energy are presented in Figures 4.77-4.86.
Alongside each map is a histogram of the superpixel relative efficiencies.
The efficiencies shown in these figures have not been corrected for pileup.
The reference CCD count rates used to generate each superpixel relative
efficiency have been corrected for cosmetic defects, including the effects
of shadowing by the framestore covers used during subassembly calibration
at MIT. The flight CCD count rates have not been corrected for cosmetic
defects, but have been corrected for shadowing by the subassembly calibration
framestore cover. In addition, each uniformity map has been adjusted to
reproduce the effect of shadowing by the flight framestore cover. This
procedure is intended to produce spatial uniformity maps which replicate
the quantum efficiency patterns that will be present in data obtained with
the flight CCDs on orbit. The number of rows in each device shadowed by
the subassembly and flight framestore covers are listed in Table 4.57.
Histogram legends in Figures 4.77-4.86
indicate the centroid and standard deviation of a Gaussian fit to each
histogram. The fitted standard deviation of the histogram provides a good
measure of the residual spatial variation in relative quantum efficiency,
excluding the effects of the flight framestore shield.
Spatial variations in relative QE are comparable to expected statistical
fluctuations for the FI CCDs, except the ratios which are affected by bad
or hot columns or pixels and border effects (especially the shadows of
frame store covers). These superpixel ratios are generally outliers in
the QE ratio histograms, and only weakly affect the Gaussian fit. These
effects may be seen in Figures 4.77-4.86.
Columns darker than their surrounding regions correspond to either bad
columns in the flight CCD or hot columns in the reference CCD, while lighter
columns typically correspond to bad columns in the reference CCD. The dark
row at the bottom of each relative uniformity map is due to shadowing by
the flight framestore cover.
Larger spatial variations are observed in the BI CCDs, and are believed
to be caused in part by relatively high charge transfer inefficiency (CTI),
exceeding 25% at higher energies. Some provision will need to be developed
to characterize this spatial nonuniformity in the two backside flight CCDs
(S1 and S3). These variations affect the quality of the Gaussian fit to
the histogram of QE ratios.
Table 4.57: Number of CCD Rows Shadowed by the Framestore
Covers
| Flight |
Position |
Framestore Cover |
| Device |
|
Subassembly |
Flight |
| w203c4r |
I0 |
4 |
7 |
| w193c2 |
I1 |
6 |
8 |
| w158c4r |
I2 |
7 |
7 |
| w215c2r |
I3 |
6 |
7 |
| w168c4r |
S0 |
6 |
6 |
| w182c4r |
S2 |
7 |
6 |
| w457c4 |
S4 |
1 |
5 |
| w201c3r |
S5 |
4 |
5 |
| w140c4r |
S1 |
6 |
6 |
| w134c4r |
S3 |
8 |
5 |
| w190c3 |
Ref. |
10 |
|
| w203c2 |
Ref. |
9 |
|
| w103c4 |
Ref. |
7 |
|
|
Figure 4.77: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device I0 (w203c4r) relative to reference device w190c3
at seven energies. Each pixel value is the ratio of the raw count rate
(i.e. uncorrected for pileup) in a 32 x 32 pixel subarray of the flight
device to the count rate in the corresponding subarray of the reference
device.
Figure 4.78: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device I1 (w193c2) relative to reference device w103c4 at
seven energies. Each pixel value is the ratio of the raw count rate (i.e.
uncorrected for pileup) in a 32 x 32 pixel subarray of the flight device
to the count rate in the corresponding subarray of the reference device.
Figure 4.79: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device I2 (w158c4r) relative to reference device w103c4
at seven energies. Each pixel value is the ratio of the raw count rate
(i.e. uncorrected for pileup) in a 32 x 32 pixel subarray of the flight
device to the count rate in the corresponding subarray of the reference
device.
Figure 4.80: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device I3 (w215c2r) relative to reference device w190c3
at seven energies. Each pixel value is the ratio of the raw count rate
(i.e. uncorrected for pileup) in a 32 x 32 pixel subarray of the flight
device to the count rate in the corresponding subarray of the reference
device.
Figure 4.81: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device S0 (w168c4r) relative to reference device w190c3
at seven energies. Each pixel value is the ratio of the raw count rate
(i.e. uncorrected for pileup) in a 32 x 32 pixel subarray of the flight
device to the count rate in the corresponding subarray of the reference
device.
Figure 4.82: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device S2 (w182c4r) relative to reference device w103c4
at seven energies. Each pixel value is the ratio of the raw count rate
(i.e. uncorrected for pileup) in a 32 x 32 pixel subarray of the flight
device to the count rate in the corresponding subarray of the reference
device.
Figure 4.83: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device S4 (w457c4) relative to reference device w190c3 at
seven energies. Each pixel value is the ratio of the raw count rate (i.e.
uncorrected for pileup) in a 32 x 32 pixel subarray of the flight device
to the count rate in the corresponding subarray of the reference device.
Figure 4.84: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device S5 (w201c3r) relative to reference device w190c3
at seven energies. Each pixel value is the ratio of the raw count rate
(i.e. uncorrected for pileup) in a 32 x 32 pixel subarray of the flight
device to the count rate in the corresponding subarray of the reference
device.
Figure 4.85: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device S1 (w140c4r) relative to reference device w103c4
at seven energies. Each pixel value is the ratio of the raw count rate
(i.e. uncorrected for pileup) in a 32 x 32 pixel subarray of the flight
device to the count rate in the corresponding subarray of the reference
device.
Figure 4.86: Uniformity
maps and histograms showing the spatial uniformity of the quantum efficiency
of ACIS flight device S3 (w134c4r) relative to reference device w203c2
at seven energies. Each pixel value is the ratio of the raw count rate
(i.e. uncorrected for pileup) in a 32 x 32 pixel subarray of the flight
device to the count rate in the corresponding subarray of the reference
device.



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Quantum Efficiency Measured
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Consistency of Relative
Please address comments and questions to Dr. John Nousek ( nousek@astro.psu.edu
)