Rotating mirror optical scanning device
DEDICATORY CLAUSE 
     The invention described herein may be manufactured, used, and licensed by or for the U.S. Government for governmental purposes without the payment to me of any royalties thereon. 
    
    
     BACKGROUND OF THE INVENTION 
     This invention relates to an optical scanning mechanism. It has a very large focal plane area coverage and can accept a large f-cone from an external imaging system. It has a scan rate of up to 200 lines per second and can generate several original scan patterns by varying the settings of the invention. 
     There are numerous mechanical scanning systems which have been built that provide one and two-dimensional image scan patterns for optical systems. These systems range from simple two-axis gimbals and rotating multifaceted cylinders to cam-actuated tilting mirrors or prisms and complex combinations of mirrors, lenses, prisms, and holographic hybrids. 
     One of these systems uses a pair of counter-rotating prisms in a tube, but this system is strongly wavelength dependent. In all such systems, there is invariably, a trade-off between the optical throughput, the scan rate, and the Field of View (FOV). This problem is particularly acute for systems which must operate at low light levels under conditions which require high (real-time) scan rates and wide fields of view. In such cases the optical designer usually abandons mechanical scan generators in favor of arrays or other non-mechanical means of image generation. However, for some spectral regions, these alternate approaches do not exist. This is true for the very far infrared and submillimeter spectral regions. Furthermore, in these regions, the minimum image resolution spot size is large compared to the visible spectral region. In order to scan an image with enough resolution cells to synthesize patterns, the FOV and the physical area covered in the focal plane must also be large. 
     SUMMARY OF THE INVENTION 
     The scanning device of the invention will accommodate a large aperture primary mirror which is necessary in order to collect the incident radiation, and the large focal plane area necessary for scene resolution, while still providing a rapid mechanical scan rate for real-time imaging. In addition, the same scanning device can generate a variety of one and two-dimensional scan patterns simply by varying the mechanical phase and rotational differences between the two rotating mirrors included in the device. Since the device of the invention uses reflective elements to make the scan, it is independent of the wavelength. The focal plane scanner utilizes two relay lenses, but they do not produce the scanning action. 
     It is an object of the invention to provide an optical scanning mechanism which can scan a large focal plane area and accept a large f-cone from the external imaging system. 
     It is another object of the invention to provide an optical scanning mechanism which scans a large focal plane area mechanically at a rate of up to 200 lines per second. 
     It is still a further object of the invention to provide a mechanical optical scanning device which is adjustable and can generate one or more scan patterns by varying the mechanical phase and the rotational velocities of a pair of rotating mirrors. 
     It is yet another object of the invention to provide a mechanical optical scanning device which is particularly adaptable to scanning a large focal plane area, generated by infrared and submilimeter imaging systems. 
     These and other objects, which will become apparent, are attained by the mechanical optical scanning device of the invention which is illustrated in the drawings appended hereto, and described in detail in the accompanying specification. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     The invention will now be described in connection with the appended drawings, wherein: 
     FIG. 1 is a perspective view of the optical scanning device of the invention; 
     FIG. 2 is a schematic plan view of the optical scanning device illustrated in FIG. 1; 
     FIG. 3 is a tunnel diagram of the optical throughput of the optical scanning device illustrated in FIGS. 1 and 2; 
     FIG. 4(a) is a graph illustrating the vertical scan mode; 
     FIG. 4(b) is a graphic representation of the horizontal scan mode; 
     FIG. 4(c) is a graphic representation of the circular scan mode; 
     FIG. 4(d) is a graphic representation of the spiral scan mode; and 
     FIG. 4(e) is a graphic representation of the rotating radial scan mode. 
    
    
     DETAILED DESCRIPTION OF THE DRAWINGS 
     Referring now to FIGS. 1, 2 and 3, wherein the scanning device 10 of the invention comprises an imaging lens 12 for directing the beam of light to be scanned into the scanning device 10. Imaging lens 12 produces a focused image on the plane in which a field lens 14 lies. The beam of light 30 is directed by field lens 14, onto the surface of a first rotary reflecting mirror 16, which is supported for rotation on a shaft 18. Each ray of the light beam 30 impinges upon a different point on reflecting means 16, and, in turn, is reflected in a second direction or path onto the surface of a second rotary reflecting means 22. As seen best, in FIG. 2, the first rotary reflecting means 16 is a mirror mounted on shaft 18 at an angle of less than 90° to the axis of the shaft so that each ray of light beam 30 which impinges upon surface 16 is reflected in an elongated elliptical path, as at 34. 
     The second rotary reflecting means 22 is supported on shaft 24 also at an angle α as indicated at 20 so that the rotary reflecting means 22 rotates in a series of planes so as to redirect the elliptical path 34 in a further elongated elliptical path, through a relay lens 28, and onto a detecting means 36. The full line and the dotted line positions in FIG. 1 and FIG. 2 represent the path of a single point or light ray 32 which travels through the scanning device. In the event that the device is to be used to scan the entire aperture of input beam 30, field lens 14 and relay lens 28 may be dispensed with. 
     As pointed out above, mirrors 16 and 22 are tilted on their axles or shafts 18 and 24 at an angle α with the axis of their rotary shafts, and their rotational speeds are synchronized with a preset phase difference and sense of rotation. Point 32 of light beam 30 is reflected from mirror 16 in a small elliptical cone as mirror 16 rotates. The axis of the cone is at an angle to the axis of rotation of mirror 16 and has an apex angle of two α. Upon reflection from the second mirror 22, a second conical movement is superimposed on reflected point or ray 32. When the rotations and phases are correctly adjusted, as illustrated in FIG. 4(b), the net angular movement of ray 32 can be controlled so that the vertical movements are substantially cancelled while the horizontal deflections are increased, to produce an elongated substantially flat elliptical path which is substantially tantamount to a straight line scanning motion. This results in the horizontal scan mode illustrated in FIG. 4(b). 
     FIG. 4(a) illustrates the vertical scan mode and is similar to the horizontal scan mode illustrated in FIG. 4(b), except that it is in the vertical plane rather than the horizontal plane. 
     A detailed mathematical analysis shows that, for a small angle α, and the pentaprism geometry of FIG. 1, the horizontal and the vertical angular deflections, θ H  and θ V  are given by the following equations: 
     
         θ.sub.H =2α[SIN (W.sub.1 T+β)+SIN W.sub.2 T] 
    
     
         θV+2αCOS 22.5° [COS(W.sub.1 T+β)+COS W.sub.2 T] 
    
     where 
     α=mirror tilt angle, same for both mirrors. 
     β=relative phase of the direction of tilt between the two mirrors. 
     w 1  =angular velocity of mirror 16 
     w 2  =angular velocity of mirror 22 
     The field of view of the focal plane scanning embodiment of the invention is established by consideration of the tunnel diagram of FIG. 3. The points (a) and (b) show the maximum coverage of the scanner for a mirror tilt angle and the indicated relative spacing of the mirrors 16 and 22 at field lens 14 and relay lens 28. 
     As illustrated in FIG. 3, this is a geometrical construction. The focal length of lens 14 is chosen to reimage primary mirror 16 at a point halfway between mirrors 16 and 22. The focal length of lens 28 is chosen to re-image the plane of lens 14 onto the detector means 36. The scan FOV is then determined by specifying the desired ratio of the primary aperture diameter to that of lens 14 for a given f/#. The diagram in FIG. 3 shows that an f/2.5 imaging system can be scanned over an 11.4° FOV if an f/1 field lens 14 and an f/2 relay lens 28 are utilized, and the focal plane diameter ratio to that of the f/2.5 primary mirror 16 is in the ratio of 1:2. 
     Each revolution of the tilted mirrors yields one complete angular cycle, consisting of one scan line across the FOV and a second scan line back to the starting point, for a total of two scan lines per revolution. Thus, an operating frequency of 6000 rpm gives 100 rps, or 200 lines per second altogether. For an image with a moderate line resolution of 50-100 lines per frame, this gives from two to four frames per second output. 
     The scanning device of the invention offers a number of advantages over other mechanical scanners. It has a wide FOV, a high scan rate, and a large f-cone acceptance capability. It can also scan very large area focal planes with little or only partial obscuring of the throughput. 
     The device illustrated in FIGS. 1, 2, and 3 can generate either horizontal or vertical line scans, as described above, but can also be adjusted to scan a two-dimensional FOV in either a rotating radial line scan or a periodic spiral scan pattern, depending upon the settings of the angular velocities and relative phases of the two rotating mirror elements. 
     As seen in FIG. 4(c), the phase and rotational speeds can be adjusted to provide a circular scan mode without modifying the structure of the scanning device itself. 
     FIG. 4(d) illustrates a spiral scan mode which may be attained, again by adjusting the speed and phases of the mirrors in accordance with the illustrated formula. FIG. 4(e) illustrates a different scanning pattern wherein a flattened elliptical path such as that shown in FIG. 4(a) and 4(b) is performed by the apparatus, but with the path slowly rotating radially above a center line to produce a rotating radial scan mode. 
     Each of FIG. 4(a), 4(b), 4(c), 4(d) and 4(e) illustrates the formula for calculating in adjusting the speeds and phases of the rotating mirrors to produce the scan pattern illustrated in each.