KAF−4320
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4
Image Acquisition
An electronic representation of an image is formed when
incident photons falling on the sensor plane create
electron-hole pairs within the sensor. These photon induced
electrons are collected locally by the formation of potential
wells at each photogate or pixel site. The number of
electrons collected is linearly dependent on light level and
exposure time and non-linearly dependent on wavelength.
When the pixel’s capacity is reached, excess electrons will
leak into the adjacent pixels within the same column. This
is termed blooming. During the integration period, the fV1
and fV2 register clocks are held at a constant (low) level.
See Figure 17.
Charge Transport
Referring again to Figure 17, the integrated charge from
each photogate is transported to the output using a two-step
process. Each line (row) of charge is first transported from
the vertical CCD to the horizontal CCD register using the
fV1 and fV2 register clocks. The horizontal CCD is
presented a new line on the falling edge of fV2 while fH1
is held high. The horizontal CCD then transports each line,
pixel by pixel, to the output structure by alternately clocking
the fH1 and fH2 pins in a complementary fashion. On each
falling edge of fH1L a new charge packet is transferred onto
a floating diffusion and sensed by the output amplifier.
Output Structure
Charge presented to the floating diffusion is converted
into a voltage and current amplified in order to drive of f-chip
loads. The resulting voltage change seen at the output is
linearly related to the amount of charge placed on the
floating diffusion. Once the signal has been sampled by the
system electronics, the reset gate (fR) is clocked to remove
the signal and the floating diffusion is reset to the potential
applied by V RD. (See Figure 4). More signal at the floating
diffusion reduces the voltage seen at the output pin. In order
to activate the output structure, an off-chip load must be
added to the VOUT pin of the device such as shown in
Figure 6.
If charge binning is desired, the charge can be combined
at the output node or it can be combined in the fH1L gate
and then presented to the output node.
Dark Reference Pixels
There are 4 light shielded pixels at the beginning of each
line. There are 4 dark lines at the start of every frame and 4
dark lines at the end of each frame. Since there are outputs
at each of the four corners, the light shield will affect the
beginning o f each line from each output, and for the first four
lines from each of the outputs. Under normal circumstances,
these pixels do not respond to light. However, dark reference
pixels in close proximity to an active pixel can scavenge
signal depending on light intensity and wavelength and
therefore will not represent the true dark signal.
Dummy Pixels
Within the horizontal shift register are 4−1/2 leading
pixels that are not associated with a column of pixels within
the vertical register. These pixels contain only horizontal
shift register dark current signal and do not respond to light.
A few leading dummy pixels may scavenge false signal
depending on operating conditions.
Figure 4. Output Architecture
Source
Follower
#1
Source
Follower
#2
HCCD
Charge
Transfer
Floating
Diffusion
VDD
VOUT
VRD
VOG
R
H1
H1
H2
H2
VLG