KAI−1020
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(fV2A, fV2B, fV1), and fast dump drivers (fFD) should
be held at the low level. This prevents unwanted noise from
being introduced into the CDS circuit.
The HCCD is a type of charge coupled device known as
a pseudo-two phase CCD. This type of CCD has the ability
to shift charge in two directions. This allows the entire image
to be shifted out to the video 1 output CDS, or to the video 2
output CDS (left/right image reversal). The HCCD is split
into two equal halves of 522 pixels each. When operating the
sensor in single output mode the two halves of the HCCD are
shifted in the same direction. When operating the sensor in
dual output mode the two halves of the HCCD are shifted in
opposite directions. The direction of char ge transfer in each
half is controlled by the fH1BL, fH2BL, fH1BR,
and fH2BR timing inputs.
Single Output
To direct all pixels to the video 1 output make the
following HCCD connections:
fH1S = fH1BL, fH2BR
ąfH2S = ffH2BL, fH1BR
To direct all pixels to the video 2 output make the
following HCCD connections:
fH1S = fH2BL, fH1BR
ąfH2S =ffH1BL, fH2BR
In each case the first 8 pixels will contain no electrons,
followed by 12 dark reference pixels containing only
electrons generated by dark current, followed by 1004
photo-active pixels, followed by 12 dark reference pixels.
The HCCD must be clocked for at least 1028 cycles.
The VCCD may be clocked immediately after the 1028th
HCCD clock cycle.
If the sensor is to be permanently operated in single output
mode through video 1, then VDD2 (pins B8, and B10) may
be connected to GND. This disables the video 2 CDS and
lowers the power consumption.
If the sensor is to be permanently operated in single output
mode through video 2, then VDD1 and VDD2 supplies must
be +15 V. The VDD1 supplies must always be at +15 V for
the sensor to operate properly.
Dual Output
To use both outputs for faster image readout, make the
following HCCD connections:
fH1S = fH1BL, fH1BR
fH2S = fH2BL, fH2BR
For both outputs the first 8 HCCD clock cycles contain n o
electrons, followed by 12 dark reference pixels containing
only dark current electrons, followed by 502 photo-active
pixels. This adds up to 522 pixels, but the HCCD should be
clocked for at least 523 cycles before the next VCCD line
shift takes place. The extra HCCD clock cycle ensures that
the signal from the last pixel exits the CDS circuit before the
VCCD drivers switch the gate voltages. This extra cycle is
not needed for the single output modes because in that case,
the last pixel is from a column of the dark reference which
is not used. See the section on correlated double sampling
for a description of the one pixel delay in the CDS ci rcuit.
Electronic Shutter
Substrate Voltage
The voltage on the substrate, pins L1 and L5, determines
the charge capacity of the photodiodes. When VSUB is 8 V
the photodiodes will be at their maximum charge capacity.
Increasing VSUB above 8 V decreases the charge capacity
of the photodiodes until 30 V when the photodiodes have
a charge capacity of zero electrons. Therefore, a short pulse
on VSUB, with a peak amplitude greater than 30 V, empties
all photodiodes and provides the electronic shuttering
action.
Substrate Voltage and Anti-Blooming
It may appear the optimal substrate voltage setting is 8 V
to obtain the maximum charge capacity and dynamic range.
While setting VSUB to 8 V will provide the maximum
dynamic range, it will also provide the minimum
anti-blooming protection.
The KAI−1020 VCCD has a charge capacity of 60,000
electrons (60 ke−). If the VSUB voltage is set such that the
photodiode holds more than 60 ke−, then when the charge is
transferred from a full photodiode to VCCD, the VCCD will
overflow. This overflow condition manifests itself in the
image by making bright spots appear elongated in the
vertical direction. The size increase of a bright spot is called
blooming when the spot doubles in size.
The blooming can be eliminated by increasing the voltage
on VSUB to lower the charge capacity of the photodiode.
This ensures the VCCD charge capacity is greater than the
photodiode capacity. There are cases where an extremely
bright spot will still cause blooming in the VCCD. Normally,
when the photodiode is full, any additional electrons
generated by photons will spill out of the photodiode.
The excess electrons are drained harmlessly out to the
substrate. There is a maximum rate at which the electrons
can be drained to the substrate.
If that maximum rate is exceeded, (say, for example, by
a very bright light source) then it is possible for the total
amount of charge in the photodiode to exceed the VCCD
capacity. This results in blooming.
The amount of anti-blooming protection also decreases
when the integration time is decreased.
There is a compromise between photodiode dynamic
range (controlled by VSUB) and the amount of