U.S. patent number 3,727,057 [Application Number 04/202,771] was granted by the patent office on 1973-04-10 for infrared detector device with a mosaic of oppositely-poled adjacent elements.
This patent grant is currently assigned to Westinghouse Electric Corporation. Invention is credited to Richard F. Higby, Mike Lauriente.
United States Patent |
3,727,057 |
Higby , et al. |
April 10, 1973 |
INFRARED DETECTOR DEVICE WITH A MOSAIC OF OPPOSITELY-POLED ADJACENT
ELEMENTS
Abstract
An infrared detector device incorporating a checkerboard
arrangement of photoconductor detector elements is disclosed.
Adjacent elements are oppositely poled, resulting in the
cancellation of background signals on any two adjacent elements,
thereby providing background discrimination.
Inventors: |
Higby; Richard F. (Severna
Park, MD), Lauriente; Mike (Clarksville, MD) |
Assignee: |
Westinghouse Electric
Corporation (East Pittsburgh, PA)
|
Family
ID: |
22751192 |
Appl.
No.: |
04/202,771 |
Filed: |
June 15, 1962 |
Current U.S.
Class: |
250/338.1;
313/531; 348/294 |
Current CPC
Class: |
G01S
3/784 (20130101) |
Current International
Class: |
G01S
3/78 (20060101); G01S 3/784 (20060101); G01t
001/16 () |
Field of
Search: |
;250/83.3IR,213,220,227,86.3,211,83.3H,83.3HP,209
;313/65,66,96,95,65A,96 ;88/1R ;178/7.2 ;338/17,18 ;244/114.3 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Quarforth; Carl D.
Assistant Examiner: Nelson; P. A.
Claims
We claim as our invention:
1. An infrared detector comprising, in combination, an insulating
supporting plate member, a plurality of photoconductive detector
elements arranged in a plurality of parallel vertical and
horizontal rows disposed orthogonally with respect to each other,
means for biasing said detector elements said elements being
arranged in checkerboard pattern and each being poled so as to
develop potential drops of opposite polarity at common output
terminals in response to infrared radiation, a plurality of
elongated spaced electrodes on said supporting plate member, all of
said first plurality of spaced electrodes being electrically
connected together to a first terminal, a second plurality of
spaced elongated electrodes mounted on said supporting plate
member, all of said second plurality of electrodes being
electrically connected to a second terminal, said first and second
plurality of electrodes being in interleaved relation, all of said
electrodes being disposed at an angle of 45.degree. with respect to
said horizontal and vertical rows, means forming an insulating film
disposed over all of said electrodes and said supporting late, said
insulating film having a plurality of small apertures therein at
spaced intervals corresponding to the centers of said detector
elements, each of said apertures lying over an electrode, and a
photoconductive film overlying all of said electrodes and apertures
and in contact with said electrodes.
Description
This invention relates to improvements in infrared detectors and
more particularly to an improved infrared detector employing the
principle of cancellation to break up the image plane into a mosaic
of point size detector elements polarized in such a manner that any
signal induced on any two adjacent elements cancel each other out
and thereby provide background discrimination.
As will be understood by those skilled in the art, the detection
sensitivity of infrared surveillance systems employing point
detectors for mechanically scanning the scenery are limited by the
spurious noise induced by background. sources. These sources
commonly referred to as scanning or sky noise, are in the form of
clouds and intensity gradients as might be found in a sky or
terrain background. A differential in energy between two
consecutive points along the line of scan constitutes a target in
the employment of these systems. Since the existence of energy
differential is not unique to real targets, but applies also to
background sources, subsequent techniques for discriminating energy
differentials is also required.
A number of techniques in general use are all characterized by one
or more disadvantages or limitations. One technique in use in the
prior art depends upon spatial differences between the target and
background sources. This is possible because the target appears as
a point source, for all intents and purposes, in the image plane of
the optical system. Background sources of point size do not emit
enough energy to be discernible because they are usually materially
cooler than the target. Therefore, background sources must have an
extended area in order to emit sufficient energy to be
detectable.
This spatial difference is exploited in prior art circuits in two
general ways, one of which is called pulse width discrimination and
the other is called space filtering. Pulse width discrimination
takes advantage of the difference in the frequency spectra produced
by the area difference between the target and background sources
when swept over by the scanning aperture. Space filtering utilizes
a reticle of alternate opaque and transparent apertures which are
essentially of point size. A chopped signal is generated by the
radiation from a point source target as it is swept across this
reticle disposed in the image plane during scanning. The electronic
system is made selective to this chopped signal. Extended area
sources do not generate this signal because of an averaging out of
the chopping due to an equal number of transparent and opaque
apertures in the scan. Thus extended area induced signals are
filtered out.
Although these techniques may at least partially suppress
background noise, they do not eliminate it and thus leave much to
be desired. In the contemporary system the reticle is used to break
up the image plane into a checkerboard pattern of point size
detector elements, the alternate ones of which are opaque and
transparent. With extended area sources of radiation background,
the averaging out of the chopping due to the alternate opaque and
transparent apertures provide a low amplitude noise type signal at
gives no particular difficulty. However, in such system the edges
of such a background area gives rise to transient signals which can
be readily mistaken for real target signals and such false signals
cannot be readily eliminated. Such a typical contemporary system is
illustrated in the drawings and is compared with the operation of
the system in accordance with the present invention.
As contrasted to the prior art systems using the reticle type
system, the present invention employs a cancellation detector
having an array of elemental detector elements arranged along sets
of parallel and horizontal orthogonal axes, adjacent elements along
each axis being alternately oppositely polarized so as to give
responses of opposite polarity when scanned by radiation from a
point source. Since any extended area source of radiation can be
considered as having an infinite number of point sources, signal
cancellation is effective at the edges of an extended source as
well as it is throughout the body of the extended source and
therefore no false target signals will be generated as the beam
sweeps across an extended area source.
Accordingly, a primary object of the present invention is to
provide a new and improved infrared radiation detector.
Another object is to provide a new and improved infrared detector
employing cancellation to eliminate signals due to background
radiation.
Another object is to provide a new and improved infrared detector
cell for use in the system in accordance with the present
invention.
The above and other objects will become apparent when considered in
connection with the accompanying drawings, in which:
FIG. 1 is a schematic representation of a typical apparatus for
scanning an infrared optical aperture over a surveillance area;
FIG. 2 is a schematic representation of a contemporary system where
the aperture is scanned over a checkerboard reticle;
FIG. 3 is a schematic representation of the spatial relation
between an extended background, a target and a detector cell
together with the associated signals and circuitry;
FIGS. 4 and 5 are views of one embodiment of the invention, FIG. 5
showing the optical portion of the detector apparatus removed from
the photoconductive assembly for clarity of illustration;
FIG. 6 is a simplified electrical circuit diagram illustrating the
operation of the invention;
FIGS. 7A, 7B, 7C and 7D are views of a second embodiment of the
invention in various stages of assembly;
FIG. 8 is a sectional view of FIG. 7D on line VIII--VIII and
looking in the direction of the arrows; and,
FIG. 9 is a representation of a greatly enlarged photograph of a
third embodiment.
The general schematic arrangement of the present invention is
illustrated in FIG. 1 wherein any suitable optical system 1 is
adapted to direct infrared radiation on a detector cell 2 which is
located in the focal plane of the optical system. The exact type of
optical system is immaterial. It is illustrated for convenience as
being a single positive lens although as very well understood in
the art a reflective type of system could be used. The optical
system 1 and the detector cell 2 are mounted in such a manner that
they can be moved in unison. The optical system 1 may be mounted in
any suitable means so that it can oscillate about orthogonal axes
for the purpose of providing the necessary scanning motion so that
the aperture of the optical system is scanned over the surveillance
area. In this connection, it should be understood that the optical
system would be mounted in the necessary manner so that it could
oscillate about the vertical axis, the oscillation being indicated
by the double pointed arrow 3 in proper time relation with slower
oscillation movement about the center of the optical axis indicated
at 4. In this manner, the aperture is scanned from side to side as
the optical axis is tilted progressively up and down. The operation
of the scanning system would be in accordance with conventional
practice and constitutes no part of the present invention. The
above is mentioned primarily to indicate that the scanning
operation of the optical system has the effect of producing the
pulsating signal in the present system much in the manner as a
light chopper produces a pulsating signal in other systems using
the contemporary checkerboard pattern reticle system.
FIG. 2 schematically illustrates the disadvantage of contemporary
systems using the checkerboard pattern reticle system wherein the
radiation from the surveillance area would be scanned across the
reticle, which corresponds to the detector cell shown in FIG. 1. It
will be seen that when a large area background, such as a cloud, is
scanned, a noise-like signal illustrated at 6 will be produced at
the output of the single detector cell used with the reticle. The
body of a cloud may be considered to include an infinite number of
reflectors spaced very close together so that the amount of energy
reflected from the cloud is comparatively high and substantially
constant as the cell is swept across the area. On the other hand,
at the edges of the clouds there is a differential in energy
between two consecutive points along the line of scan and this
causes the generation of transient signals 7 and 8 which cannot
readily be distinguished from a signal from a real target such as
that indicated at 9.
The advantage of the present invention over the system
schematically symbolized in FIG. 2 will be readily apparent from a
comparison of the latter figure with FIG. 3. The scanning system
may be the same as that schematically represented in FIG. 1 and the
detector cell 2 will be made in accordance with one of the
embodiments of the present invention. Because of the cancellation
technique, hereinafter pointed out in greater detail, the point
size detector elements of the detector cell 2 are polarized in such
a manner that any signal induced on any two adjacent elements
cancel each other and therefore only the noise-like signal of low
amplitude, such as that indicated at 10, will be developed in the
output circuit of the detector cell 2. This is to be compared with
the signal 6 of FIG. 2. On the other hand, a point size target 11
will develop an oscillating signal 12 which can be clearly
recognized as that coming from a point size target.
In the first embodiment, shown in FIGS. 4 and 5, the detector cell
2 has associated therewith a plurality of light pipes 13 having
entrance pupils 14 and exit pupils 16 adjacent to a supporting
structure 17 on which are disposed a plurality of radiation
sensitive elements 18' and 18". The areas and dimensions of these
elements correspond approximately to the areas and dimensions of
the exit pupils 16 of the light pipes. The use of light pipes in
infrared detectors is more fully explained in a copending
application by Francis J. Keisler and Richard F. Higby entitled
"High Resolution Radiation Detector", Ser. No. 57,177, filed Sept.
20, 1960 now U.S. Pat. No. 3,110,816, dated Nov. 12, 1963 and
assigned to the assignee of the instant application.
In that copending patent application the advantages to be obtained
by the use of light pipes having exit pupils smaller than the
entrance pupils is described in detail. Such construction provides
concentrations of radiation on the detector elements and also
provides space to make the electrical connections. As will appear
from the subsequent description, the light pipes shown in FIGS. 4
and 5 are associated with the first and second embodiments of the
invention while the third embodiment, illustrated in FIG. 9, does
not require the use of these light pipes.
Referring to FIG. 6, it will be noted that the output signals are
delivered by the leads 19 and 21. Lead 19 is connected to one side
of detector elements 18' and lead 21 is connected to the opposite
sides of alternate detector elements 18" of the upper row and to
the same corresponding sides of the elements of each of the other
transverse rows. In other words, lead 19 is connected to alternate
sides of adjacent cells arranged in a checkerboard pattern while
lead 21 is connected to the other sides of alternate cells in the
checkerboard pattern. Lead 22 is connected to the other sides of
the remaining alternate elements. As shown in FIG. 6, a source of
direct current biasing voltage, such as the battery 23 has its
positive terminal connected to lead 22 and its negative terminal
connected to the lead 21, which is also connected to ground at 24.
In other words, lead 19 is common to one side of all of the
detector elements and alternate detector elements disposed in
vertical and horizontal rows are oppositely polarized. The
positively polarized detector elements are designated 18' and the
negatively polarized detector elements are designated 18".
It will be readily understood that if the elements 18', 18", which
are identical but oppositely polarized photoconductive elements,
receive no illumination, or are illuminated uniformly with
electromagnetic radiation such as infrared light, the output lead
19 will be at a constant potential which will be substantially
one-half the potential of the battery 23. If the total illumination
on detector elements 18' becomes greater than the total
illumination on detector elements 18" so that their conductivity
increases, the potential of lead 19 rises toward the positive
potential of lead 22 whereas, if the total illumination on detector
elements 18" is greater than that on the elements 18' the potential
difference between leads 21 and 19 is decreased and, in effect,
lead 19 becomes less positive. In this way, as the elements 18' and
18" are alternately illuminated, such as when being scanned by
infrared radiation through a scanning aperture, the amplitude of
the voltage on lead 19 alternately varies in positive and negative
directions about some average value to provide an output analog
signal.
In manufacturing the detector of the present, the electrode pattern
may be laid down on the detector substrate 17 by a photoetching
process. The detector elements 18' and 18" may then be laid down in
small squares either by photoetching, scribing or some other
suitable process. One significant aspect of the apparatus of FIG. 5
is the interleaving of the electrodes such that no crossovers occur
and the desired polarity reversals occur at every element. The
sensitivity of the detector of FIGS. 4 and 5 is augmented by the
integrated light pipes 13 which, as previously mentioned, provides
space between the exit pupils 16 for interconnecting the signal
electrodes.
Particular reference is made now to FIGS. 7A, 7B, 7C and 7D, which
together illustrate a second embodiment of the invention. Upon a
substrate supporting member 17 of suitable insulating material
there is supported two sets of interleaved bias electrodes, the
electrodes of one group being electrically connected together and
designated 26, 27 and 28 and having a common terminal strip 29 and
the electrodes of the other group being designated 31, 32, 33 and
34 and having a common terminal strip 36. The electrodes and
terminal strips may be in the form of a gold film plated upon the
substrate 17. An insulating film 37 (FIGS. 7B and 7D) is then
deposited over the gold film electrodes. The insulating film 37
covers substantially the entire surface of the substrate 17. A
common electrode member 38 somewhat in the form of an egg carton
separator and having spaced square recesses 39 therein, is then
secured in any convenient manner over the insulating film 37. The
common electrode member 38 has a terminal strip 41. As will be
noted the square recesses 39 are spaced in a plurality of parallel
horizontal and vertical rows in such a manner that substantially
the center of each of the square recesses 39 lies over one of the
electrodes 26, 27, 28, 31, 32, 33 or 34. A plurality of small holes
42, one in each recess 39, are then etched through the insulating
film 37 exposing the common electrode 38 as shown in FIGS. 7B, 7C
and 7D. A photosensitive film, shown at 43 in FIG. 7D is then laid
over the entire assemblage in block fashion. The photoconductive
film 43 flows into the recesses 39 and through the holes 42 into
contact with the finger electrodes 26, 27, 28, 41, 32, 33 and 34,
thus forming photoconductive cells, in general, similar to those of
FIG. 1. The terminal strip 41 of the common electrode 38
corresponds to the output lead 19 of FIG. 6. The terminal strips 29
and 36 are connected, respectively, to terminals corresponding to
leads 22 and 21, respectively, of FIG. 6 to the positive and
negative terminals of a suitable direct current source (not shown)
to give a circuit configuration similar to that shown in FIG. 6 and
providing a checkerboard pattern of adjacent alternately oppositely
biased detector cells similar to that shown in FIG. 5.
As the detector apparatus is scanned and the target image moves
across member 43 in either a horizontal or a vertical direction,
areas of the sensitive member 43 opposite the holes 42 which are
alternately biased at different polarities, as previously
described, are successively illuminated by the relatively high
intensity radiation of the target source. Accordingly, a signal
which varies alternately from positive to negative is generated in
the output circuit as infrared radiation from the target is scanned
across the member 43.
Particular reference is made now to FIG. 9 in which a third
embodiment of the invention is shown. The detector of FIG. 9 is
seen to consist of sets of interleaving hairlike electrodes in
contact with a photoconductive film 44. One set of electrodes 46a
serves as common biasing electrodes and is connected to a terminal
strip 46, corresponding electrically to the lead 19 of FIG. 6. A
second set of electrodes 47a are connected to a terminal strip 47,
which might correspond electrically to the lead 22 of FIG. 6, while
a third set of electrodes 48a are connected to a terminal strip 48.
This terminal strip corresponds electrically to lead 21 of FIG. 6.
Similar to the previous embodiments, the terminal strip 46 serves
as the signal output terminal while the terminal strips 47 and 48
may be connected to the positive and negative terminal of a direct
current source, not shown. It will be seen that between each
positive and negative electrode there is a biasing electrode 46a.
Because of the hairlike size of the electrodes 46a, 47a and 48a and
the manner in which they are connected to their terminal strips it
is not necessary to use the light pipe arrangement as is used with
the two previous embodiments. It should be understood that the
electrodes 47a and 48a, which must pass either under or over the
terminal strip 46, are insulated therefrom in any suitable manner.
The photoconductive film 44 is laid over the electrodes 46a, 47a
and 48a in conductive relation therewith thereby forming strip-like
detector cells. It will be seen that as these strip-like cells are
scanned as the infrared radiation from a point target moves across
the cells the alternately positively and negatively biased
electrodes will be successively illuminated with the result that an
alternating current signal, having a frequency determined by the
rate of movement, is produced. On the other hand, since the spacing
between adjacent positive and negative electrodes is substantially
equal to that of the diameter of the blur circle of the optical
system, background radiation such as that from a cloud, will
illuminate two or more cells simultaneously thereby producing
potentials which tend to cancel out and thereby produce no
substantial output signal.
The invention contemplates the use of filtering circuits, if
desired, to filter out undesired extraneous alternating current
components of the detector output signal caused either by targets
or by background environment.
In FIG. 9 preferably the bias electrode span, that is, the distance
between the positive and the next adjacent negative electrode is
substantially equal to the blur circle of the imaging system.
Whereas the invention has been shown and described with respect to
some embodiments thereof which give satisfactory results it should
be understood that changes may be made and the equivalent
substituted without departing from the spirit and scope of the
invention.
* * * * *