MIT/Lincoln Labs CCID20 W7C1 CCD Test Results
This is the fourth standard epi, thinned, backside MIT/Lincoln
Labs 2Kx4K CCD to be characterized in the UCO/Lick detector lab. It is
very similar to other standard epi CCID20s tested at Lick.
A summary report
is available. Noteworthy points include:
- Brick wall pattern. With
this device we did some tests of the amplitude of the brick wall pattern
as a function of temperature. As the report shows a dramatic reduction
in the pattern is possible if the CCD can be operated at higher temperature.
Further measurements on other devices will occur.
- CTE. Near perfect CTE is
achieved using the serial and parallel clocks which generate low spurious
charge. This is typical of Lincoln CCDs.
- Read Noise. Read noise is
around 2 electrons. This is as good as or
better than any thin CCD in the world.
- Low Level Traps. Only four
low level traps were found using charge pumping. This is a very
small number for such a large device and is evidence of Lincoln's
excellent processing capabilities.
- There is a small "dimple" in the CCD which
is about 2mm in diameter. This is probably caused either by a void in the
epoxy which attaches the thinned CCD to its supporting silicon wafer or
by a problem in the thinning itself. We have not measured the physical
depth of the depression but it is not likely to be more than a few microns
deep.
Original postscript files are available from our anonymous
ftp server and these provide better resoultion and clarity than is
usually possible on a web page. Check the INDEX
file for a description of what the other files contain. Here are a few
figures to illustrate device highlights:
- QE curve
- This is a pretty typical QE curve for the CCID20s. The
QE is an average over a fairly large portion of the CCD, so this result
is an average over the brickwall variations.
- Surface plot
- The CCD has a bow and a twist. The peak-to-peak variation
is about 27 micrometers. This does not include the "dimple" which
is probably caused by an epoxy void.
- Brick wall versus Temperature
- This plot shows the dramatic change in the brick wall
pattern amplitude with temperature. Other tests show that the amplitude
continues to decrease as the temperature is raised.
- Dimple
- The small depression in the CCD about 2mm in diameter
is seen in images only at very long wavelengths where the interference
pattern is changed.
This plot shows the QE measurement
made at a device temperatures of -130°C. It seems a little lower at the
peak than other devices we've tested recently (compare W20C1
or W6C1),
but not by much. We've found that the QE can be somewhat temperature sensitive,
especially in the less sensitive areas of the brick wall pattern. So this
result will change a little with temperature, with the QE increasing with
increasing temperature.

The two plots shown here are
the same data set. The second plot is an edge-on view to better show the
full extent of the curvature and the twist. The CCD connector is along
the right edge. The laser beam used to measure the surface shape was badly
distorted by the small "dimple" in this CCD, so that region of
the device was not measured and the dimple does not show in these plots.

Edge-on view of same data set as above.

This is a series
of line plots across the CCD showing the sensitivity variations known as
the brick wall. The four curves show the same row in four separate images
obtained when the CCD was at the indicated temperatures and they illustrate
the change in sensitivity with temperature. All of these data were obtained
at 6500Å. Other tests indicate that the amplitude of the sensitivity variations
will continue to decrease with increasing temperature. Since these CCDs
don't have MPP the dark current is certainly a problem at -100°C and above.
We have not yet begun to investigate whether or not dynamic dark suppression
will help us work at higher temperatures with low dark and low noise.

This 9000Å interference
fringe image shows the small section of the CCD in the region of the apparent
depression. The area is roughly 130 pixels or 2 mm in diamter.
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