Infrared chopper using binary diffractive optics

Abstract

A method uses an infrared imaging system to produce an image of a scene. Actual infrared radiation from the scene is detected to form a biased signal representing the radiances of objects wiithin the scene, and the biased signal is diffracted by causing rays of the radiation to pass through an array of lenslets at angles devitated from their normal path. The array includes an infrared transmissive deformable film which retains a pattern stamped into it, the pattern including a plurality of the diffracting lenslets. The diffracted and defocused radiation is detected to form a reference signal, the reference signal is subtracted from the biased signal to obtain an unbiased signal, and an image is generated and displayed in reponse to the unbiased signal.

Description

BACKGROUND OF THE INVENTION

1. Field of the Invention

This invention relates to a chopper formed in a plastic sheet for use primarily in forward looking infrared (FLIR) systems and principally, but not limited to such systems, of the type utilizing uncooled ferroelectric infrared pyroelectric detectors.

2. Brief Description of the Prior Art

Forward looking infrared (FLIR) systems generally utilize a detector and a chopper system in conjunction with the detector for calibration of the detector. Such calibration is generally performed on-line and between detector scanning operations. Prior art infrared detectors have generally been of the cooled variety, operating at temperatures in the vicinity of liquid nitrogen, about 77° K. More recently, FLIR systems have been developed which use uncooled detectors, such systems being preferred when sufficient sensitivity can be obtained therefrom. An uncooled detector system utilizing a ferro-electric detector is intrinsically a differencing detector whose signal is the difference between that of the viewed scene and that of a reference source. In order to minimize dynamic range problems in the detectors, it is desirable to match the reference flux as closely as possible to the average scene flux. This is typically accomplished with the chopper which alternately permits the detector to view the scene and then view a reference source representing the average scene flux.

For purposes of minimizing the scene flux/reference flux delta, some FLIR systems have used as a reference source an image of the system exit pupil or an approximation of the system exit pupil. The most simple technique to approximate the exit pupil is to defocus the optical system. In the present day systems, this is accomplished in one of two ways, these being either (1) with a thick flat plate which is cut out in appropriate areas to pass the scene radiation, whereby, in solid areas, an optical defocus occurs, resulting in a pupil approximation or (2) with a solid flat plate which is covered with small ground lenslets in a pattern matching the solid area of a scanner, these lenslets accomplishing the defocus.

A problem with prior art choppers of the second type described above has been cost. In order to provide a chopper of the above described second type having a plurality of lenslets, it has been necessary to grind the lenslets individually, generally in germanium, to provide a predetermined pattern. Such prior art choppers have also been fabricated using binary diffractive optic pattern generated photomasks in conjunction with a high precision laser writer followed by etching of the desired lens patterns into the germanium wafer. Such processes have been costly. It is therefore desired to provide choppers at greatly reduced cost, preferably at a small fraction of the present cost.

SUMMARY OF THE INVENTION

In accordance with the present invention, there is provided a chopper and a method of fabrication thereof which meets the above noted economic goals. The chopper is designed for rotation about its central axis.

Briefly, the chopper in accordance with the present invention is fabricated by initially generating a photomask. The photomask is generated in conjunction with software, the preferred software being set forth herein in the APPENDIX. The software, which uses the language AutoLISP by AUTOCAD, consists of four macro routines which generate an exact scale graphical pattern of the lens array. Several lens design and chopper system variables are input and the software generates a two level data file of the graphical pattern.

Upon initiation of the first macro, the operator is queued for the design variable and then performs the calculations generating the spiral shaped boundary and fills the space within the boundary with an array of Fresnel phase plate lens structures. Several operator design inputs are required during the construction of the file. Once the first macro is loaded, all remaining macros self-load and pass calculated data to the next macro.

Each macro routine is summarized as follows:

SPIRAL.LSP generates the spiral shaped boundary which is sized to modulate the detector for a specific period of the detector sampling time. User inputs are several detector and chopper wheel assembly shape parameters. The spiral is generated using an Archimedes spiral math function.

BDO.LSP generates a single unit cell lens containing all of the lens structure. User inputs are the index of refraction of the substrate, lens diameter, spherical radius and design wavelength. The unit cell lens structure is generated using equations that model wavefront diffraction theory.

PGON.LSP takes the single circular lens and trims it to a hexagon shaped pattern for perfect nesting of the lenses without overlap or gaps. There are several operator steps to identify which segments of the lens to eliminate.

BDOMATRIX.LSP generates a honeycomb array of hexagons and blocks the hexagon shaped unit cell into each hexagon of the array.

The software accordingly generates a mask having the lens design to be finally stamped onto the chopper element as explained herein below.

A silicon wafer is then etched by reactive ion etching, using the photomask to provide the pattern, resulting in a silicon wafer master of the chopper pattern with regions in the shape of lenslets to be formed of desired dimension. The chopper pattern on the silicon wafer is then replicated with a hard material which can be easily stripped from the silicon wafer without damaging either the wafer or the hard material, such material preferably being film (index of refraction=1.52) and a wavelength of 10 μmeters, the lens structure depth is approximately 9 μmeters (0.00035 inch). Success has been achieved at 0.003 inch film thickness over the environmental temperature spectrum of the sensor without distortion of the small lens structure shapes.

The system is designed to operate in the 8 to 13.5 micron range and the APPENDIX is designed for operation in this range. Accordingly, the individual lenses are fabricated for operation in this range by the software. The software is designed for an individual lens, each lens having a perimeter preferably in the shape of a hexagon. A plurality of equally sized such hexagons are positioned on the film within an envelope in the shape of a spiral with the radius increasing proportional to the angle of rotation. An involute spiral and Archimedes spiral are the preferred envelope shapes. The hexagonal shape is preferred because hexagons can be fitted together such that they cover all of the area within the involute or spiral with no spaces between lenses.

The software generates two file layers. The first file layer is the spiral shaped pattern and the second layer is the array of hexagons. The hexagon file layer contains a hidden layer which compresses the file to a manageable size. These two files are downloaded to a database pattern compiler which translates the data into a format that is readable by the laser patterning system which then fabricates the photomask by writing the pattern onto the surface of an emulsion covered glass slide, the emulsion being, for example, AGFA photomask plates, Part No. PF-HD. There are many different types of emulsions that can be used and these would be apparent to one skilled in the art.

The hexagon array file layer is generated by the software in a rectangular window shaped pattern which overlies the spiral file layer. The hexagons that are completely exterior to the boundary of the spiral are eliminated from the file by the operator to reduce the file size. Those lens cell structures that stagger the spiral boundary and all those within the boundary are printed by the photomask writing equipment. The portion of the lens structure that falls external to the spiral is hidden by the boundary of the spiral file when the photomask is fabricated and thus it is not necessary to trim this lens structure away.

Each individual lens is a diffractive structure designed to defocus incident energy by a predetermined amount. The purpose is to achieve a defocused image of the exterior scene for use as a reference source for image differencing.

The exact shape of each lens is determined by the modulo π behavior of the desired wavefront deformation. FIG. 3 shows this modulo π behavior wherein the resultant shape for the individual lens is a concentric grating with grating depth determined from $$ T ⁡ ( r ) = T opt · [ Ψ F ⁡ ( r ) 2 ⁢ π + 1 ]

where T opt is the optimum thickness for a 2π phase shift, and is given by T opt =λ/Δn, and Ψ F (r) is the desired radial phase shift function. Normally, Δn is the deviation of the refractive index of the zone material from that of the surrounding medium (air) and λ is the design wavelength.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a chopper in accordance with the present invention;

FIG. 2 is an enlarged view of one of the hexagonally shaped lenslets of FIG. 1 ; and

FIG. 3 is a graph of the phase shift function for a Fresnel phase plate.

DESCRIPTION OF THE PREFERRED EMBODIMENT

The present invention is similar to the second technique discussed above, however the ground lenslets on germanium in the shape of an involute are replaced with an array of lenslets formed from binary diffractive elements on a film. This array performs the same function as the ground lenslets, but is much easier and economic to fabricate. The chopper uses a lenslet array composed of binary diffractive elements to perform the uniform defocusing required for calibration. The purpose of the lenslets is to defocus the radiation falling on the detector during the scan dead period of the imaging system. This defocused radiation is an approximation of the pupil irradiance and is used for differencing.

The chopper is fabricated by generating a photomask. The photomask is generated in conjunction with the software set forth herein as APPENDIX The software controls a laser which etches out the programmed pattern on a standard mask material, preferably AGFA Photomask Plates Part No. PF-HD. The mask now contains the mask pattern and, accordingly, the lens design to be ultimately stamped onto the chopper element. A silicon wafer is then etched through the mask by reactive ion etching in standard manner to provide a master of the chopper lens pattern on the silicon wafer. The chopper pattern on the silicon wafer is then replicated with a hard material which can be easily stripped from the silicon wafer without damaging either the wafer of the hard material, preferably a thin layer of silver of about 500 Å over which is electro-plated the nickel to a depth of at least 0.10 inch. The nickel replication of the pattern on the silicon wafer is then separated from the silicon wafer by placing the silicon pattern with silver and nickel layers thereon in a bath which removes the silver selectively to the nickel, preferably photoresist, although gold film provides a superior mask at added expense, the separated replication then being used in conjunc-tion with a heavy press as a stamp to stamp the lens pattern into individual sheets of an infrared transmissive material, preferably flexible film which is preferably polyethylene. The infrared transmissive material is preferably heated prior to stamping so that the pattern on the stamp is more easily impressed into the film. The film with the lens pattern thereon is the chopper element. Such chopper elements can be continually stamped out on individual sheets of the film in conjunction with the silicon wafer and the heavy press which drives the silicon wafer into the film, as above described, the silicon wafer operating as a mold or die.

The system is designed to operate in the 8 to 13.5 micron range and the APPENDIX is designed for operation in this range. Accordingly, the individual lenses are fabricated for operation in this range by the software. While the software is designed for an individual lens, a plurality of such lenses are positioned on the film in a predetermined pattern, preferably within an involute or spiral.

FIG. 1 shows a chopper in accordance with the present invention which has been fabricated in accordance with the present invention. There is shown a chopper 1 having a plurality of lenslets 3, each lenslet being in the shape of a hexagon an being about 0.2 inches across opposing sides. The lenslets 3 are of the same dimensions and are positioned to be interfitting with no spaces therebetween. The lenslets 3 are disposed within an involute 5 . The lenslets 3 are impressed into a polyethylene film (not numbered) having a thickness of at least 0.10 inch which surrounds the involute 5 . An aperture 7 is disposed at the center of the chopper 1 for securing the chopper to a device which will rotate the chopper in standard manner.

Referring now to FIG. 2 , there is shown an enlarged view on one of the lenslets 3 of FIG. 1 . FIG. 3 shows how a cross section through the lenslet would appear. The lenslet is essentially a binary Fresnel zone plate encoding phase information required for focusing (or defocusing, in this case) the scene flux.

Though the invention has been described with respect to a specific preferred embodiment thereof, many variations and modifications will immediately become apparent to those skilled in the art. It is therefore the intention that the appended claims be interpreted as broadly as possible in view of the prior art to include all such variations and modification.

Claims

1. A method for producing an image of a scene, using an infrared imaging system, comprising the steps of;(a) detecting the actual infrared radiation from said scene to form a biased signal representing the radiances of objects within said scene; (b) diffracting the infrared radiation emitted by said scene by placing an array of diffracting lenslets so that rays of said radiation pass through said lenslets at angles that are deviated from their normal path, said array including an infrared transmissive deformable film which has stamped thereinto a pattern that includes a plurality of said diffracting lenslets, and which retains the pattern stamped thereinto; (c) detecting said defracted and defocused radiation to form a reference signal; (d) subtracting said reference signal from said biased signal to obtain an unbiased signal representing radiance difference emitted by said scene; and (e) displaying an image generated in response to said unbiased signal.

2. The method of claim 1, wherein said step of detecting said defracted and dofocused radiation is carried out with an infrared detector; and wherein said diffracting step causes a uniform average radiance of said scene to be irradiated upon said infrared detector.

3. The method of claim 1, wherein said step of diffracting comprises moving said array of lenslets through sequential portions of a beam of radiation emitted by said scene.

4. The method of claim 1, wherein said lenslets confined within a spiral shaped arragement.

5. The method of claim 4, including the step of configuring said lenslets so that each is hexagonal.

6. The method of claim 1, including the step of selecting a polymeric material as said film.

7. The method of claim 6, including the step of: selecting polyethylene for use as said polymeric film.