On 2004-December-24, an ACA dark current calibration was performed. This consisted
of 5 pointings at slightly offset (2 arcmin) attitudes. At each pointing, two
full frame readouts were performed, one with a 5 second integration and one
with 10 seconds, giving a total of 10 full frame readouts. For each
integration time, the 5 images were median filtered on a pixel-by-pixel basis
to remove star images. Then the 5-second median-filtered image was subtracted
from the 10-second median-filtered image to remove dark current accumulation
during the readout period. This is important as it takes approximately 8
seconds to read out a CCD quadrant. Finally, the dark current image was
converted from counts/integration to electrons per second (e-/s).
Standard processing was used to reduce the data, the same as used for previous calibrations. This calibration was the sixth ACA dark current calibration since the ACA CCD operating temperature was reduced to -15C in July 2003. Comparison to previous calibrationsThe first in-flight ACA dark current calibration was performed on 1999-Aug-11 (1999:223) during Orbital Activation and Checkout (OAC) while Chandra's Sunshade Door was closed. We tabulate and plot results from each flight calibration below.Basic statistics The table below gives a summary of the statistical properties of the
pixel dark current values. The 'Peak' is calculated by fitting a 2nd order
polynomial to the histogram values within 5 e-/s of the median, and then
quoting the peak of the fitted polynomial. The 'Mean near peak' is
the mean for pixels with a dark current within 5 e-/s of the median.
The statistics above show the significant effect of the CCD cooldown
to -15C in July 2003. There was little change in the peak dark current
between OAC until then, and also since then. The number of "warm"
(> 100 e-/s) and "hot" pixels (> 3000 e-/s) appears to be increasing
fairly linearly with time. Hot pixels are flagged as bad
in the star selection process. A plot of the fraction of pixels
which are warm versus time is shown below, where the break in behaviour
in 2003 is clearly seen.
Differential histogramThe plot below shows the differential distribution of dark current values, in the number of pixels per 1.0 e-/s bin. The factor of 10 increase in warm pixels since OAC is evident in the tail above ~30 e-/s. For clarity, only the OAC calibration and the calibrations since mid-2003 are shown in this and following plots.The graph below shows the same data, plotted on a linear scale near zero.
There is a substantial non-gaussian tail of negative dark current values.
It is not clear if this is real or a processing artifact. The OAC dark
calibration shows only a gaussian tail consistent with electronic
read-out noise.
Cumulative histogramBelow, the cumulative histogram is shown, indicating the fraction of pixels with dark current greater than a given value.ImplicationsThe CCD cooldown to -15C, which reduced the overall dark current by about a factor of 2, has effectively removed almost 2 years of CCD dark current degradation, as measured by the fraction of warm pixels on the CCD. However, the latest dark current histograms are clearly different to the OAC calibration: pixel-to-pixel dark-current variations are now larger because of the high dark current tail of the distribution.Comments or questions: Aspect Help Last modified: 12/27/13 |