derivative measurements in the processor. The whole
process is identical to quadruplex correlation detec-
tion. techniques described by the illustrations in
Figures 4 and 5.
AUTOMATIC OPTICAL SYSTEM
A completely automatic stereo-image matching
system must have the capability of detecting and
correcting image misalignment and distortion as well
as controlling the aperture size of the correlator. Such
a system is illustrated in Figure 8. The major part of
the system is the multi-aperture correlator shown in
the previous figure.
Image distortion correction is accomplished by
means of a servo-driven anamorphic zoom system
that is placed between the transform and imaging lens
in the correlator. The system contains the necessary
cylindrical and spherical lens elements to accommo-
date for first-order image distortion.
The correlator aperture is controlled by a servo-
driven zoom lens system. Aperture control helps to
maintain a constant loop gain through the system. It
is required for accurate automatic stereo-image
matching. Besides controlling the aperture, the zoom
system conserves laser power. The zoom technique
maintains a constant power level in the entrance aper-
ture of the correlator.
Aperture
Zoom Control X and Y
Collimated Alignment Control
Laser Beam Signals
Sh Î
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dno
7 1
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Photo 1
T-Lens
Anamorphic Image
Distortion Correction
System
Image Scanner
Photo 2
The X and Y photo alignment servo-driven car-
riages are not shown; however, the error signals are
labeled and their function is depicted graphically in
terms of photo 1.
ELECTRONIC CORRELATION
Present stereo image electronic correlation systems
almost universally use flying-spot scanners as an inte-
gral part of the system. The flying-spot scanners con-
vert the pictorial information in the stereo diaposi-
tives to electrical signals that are processed by the
electronic correlator. A description -of the electronic
image correlator, therefore, necessarily includes the
scanner system. Indeed, the operational characteris-
tics of the image correlator are usually limited by the
performance of the flying-spot scanners.
The basic elements of a flying-spot scanner correla-
tor are shown in Figure 9. Each channel of the dual
flying-spot scanner system contains a scan signal
generator, a cathode-ray tube (CRT), a transfer lens,
and a phototube. The dynamic performance of the
scanner is illustrated in the drawing. The CRT gen-
erates a scanning spot that moves in a fixed pattern
called a raster; the scan signal generator controls the
size and form of the raster. The transfer lens images
the scanning spot and raster in the plane of the stereo
diapositive. As the scanning spot moves across the
Signal
Processor
Multi-Aperture
Correlator Output
Signals
Scanner Vom
Synch. Signals
Distortion
Detector
I-Lens Quadrant Lens
and Detector Assembly 2
(es
AA A
NAVAS
«T x
v
Beam Cr ss
Expander N
-
77 f). ZA \ \
IN
M /1 / = N
ke A
3 =
x ~
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IN - E.
> a
~ Alignment
DS £5 Detector
/ s
/ ^
Beam -d--
Splitter
O- Lens
Figure 8 Multi-Aperture Optical Stereo Image Matching Correlator S ystem
THERMAL MAPPING
77