Compact Wide Field-of-View Optical Imaging Method Capable of Electrically Switching to a Narrow Field of View

Abstract

An optical system that images a scene at two different fields of view, with switching between fields of view enabled by switchable mirrored surface is disclosed. A voltage change across the switchable mirror element generates a change in the reflection and transmission properties of the element, such that the element switches between a mirror state and a lens state. When nested in an annular reflective optic system of a given field of view, the switching element enables the opening of an additional optical path through the center of the reflective optics where a set of refractive optics are assembled into an imaging system for a second field of view. This dual field-of-view system changes field of view with no mechanical movement.

Claims

1. A compact wide field-of-view optical imaging method capable of electrically switching to a narrow field of view, comprising: imaging a distant object through a wide field-of-view aperture stop; first refracting said image through a meniscus lens; refracting said image from said meniscus lens through a doublet lens element; refracting said image from said doublet lens element through the aperture of a lens having an aspheric departure on its back surface; refracting said image from said lens having an aspheric departure on its back surface through the aperture of a lens having a flat front surface and a curved back surface, wherein a switchable reflective surface is disposed onto the back surface of said lens having a flat front surface and a curved back surface; and focusing said image from said aperture of a lens through said switchable reflective surface towards an image plane of a sensor array when said switchable reflective surface is switched to a clear state.

2. The compact wide field-of-view optical imaging method capable of electrically switching to a narrow field of view according to claim 1, wherein when said switchable reflective surface is switched to a mirror state, an alternate narrow field-of view image is reflected from alternate annular folded optics by said switchable reflective surface in said mirror state towards said image plane of said sensor array.

3. The compact wide field-of-view optical imaging method capable of electrically switching to a narrow field of view according to claim 1, further comprising the step of disposing a cover plate for electrode attachment and mechanical stability of the switchable reflective surface.

4. The compact wide field-of-view optical imaging method capable of electrically switching to a narrow field of view according to claim 1, wherein said switchable reflective surface is based on either liquid crystals or electrochromic switchable materials capable of switching between mirror and clear states based on switching an electrical control voltage signal.

5. The compact wide field-of-view optical imaging method capable of electrically switching to a narrow field of view according to claim 1, further comprising the step of disposing a cover glass for the sensor array.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0007] Additional advantages and features will become apparent as the subject invention becomes better understood by reference to the following detailed description when considered in conjunction with the accompanying drawings wherein:

[0008] FIG. 1 shows an exemplary optical raytrace of the imager in the narrow FOV mode whereas the switchable surface is in the reflective mirror state and the optical path to the detector is routed through the annular folded optics.

[0009] FIG. 2 is a table of the raytrace parameters for the imager with the narrow FOV path shown in FIG. 1.

[0010] FIG. 3 shows an exemplary optical raytrace of the imager in the wide FOV mode whereas the switchable surface is in the transmissive clear state and the optical path to the detector is routed through the lenses nested in the hole of the annular folded optics.

[0011] FIG. 4 is a table of the raytrace parameters for the imager with the wide FOV path shown in FIG. 3.

[0012] FIG. 5 is a close-up view of the switchable surface in the mirror state, where the dashed line represents a light ray that follows the narrow FOV path through the annular reflective optics and reflects off the switchable surface to arrive at the image plane.

[0013] FIG. 6 is a close-up view of the switchable surface in the clear state, where the dotted line represents a light ray that follows the wide FOV path through the refractive optics and transmits through the switchable surface to arrive at the image plane.

DETAILED DESCRIPTION

[0014] In one aspect, FIG. 1 shows an exemplary optical raytrace of the imager in the narrow FOV mode whereas the switchable reflective surface is in the mirror state and the optical path to the detector is routed through the annular folded optics. Light from a distant object enters the narrow FOV layout through an annular window 6, which is ultimately constricted by the aperture stop 7 behind it. As tabulated in FIG. 2, the window 6 can be fabricated from ZnS material and both an outer and an inner aperture diameter define the limits of the annular window. In this example, window 6 can have outer and inner diameters of 100.5 mm and 65 mm, respectively, and the aperture stop 7 can have outer and inner diameters of 100 mm and 70 mm, respectively. The static reflecting surfaces 1, 2, and 3 are arranged in an annular configuration concentric with the stop annulus, with the largest diameter reflecting surface 1 facing the distant object to be imaged. Reflecting surface 1 has an outer diameter aperture that can be 104.5 mm and an inner diameter that can be 66 mm. Light passing the stop 7 reflects from surface 1 and proceeds toward surface 2, which is facing surface 1 and has outer and inner aperture diameters that can be 68 mm and 40 mm, respectively. Light reflected from surface 2 subsequently reflects toward surface 3, with outer and inner aperture diameters that can be 66 mm and 30 mm, respectively. With each reflection, the light changes direction and gradually approaches the central axis of the annulus, so that the aperture of each subsequent surface has a smaller outer diameter.

[0015] Surfaces 1, 2, and 3 additionally have a radius of curvature (ROC) and aspheric attributes that help the light rays to properly form an image. The ROC values for surfaces 1, 2, and 3 can be respectively, 93.58 mm, 45.55 mm, and, 70.36 mm. The aspheric terms modify the curvature of the surface according to the equation for sag (linear departure from the vertex plane) z:

[00001]$z=\frac{r^2}{R+\sqrt{R^2-\left(1+k\right).Math.r^2}}+A_1.Math.r^4+A_2.Math.r^6+A_3.Math.r^8+A_4.Math.r^{10},$

[0016] where r is the radial distance from the vertex, R is the radius of curvature, k is the conic constant, and A.sub.n indicates aspheric coefficients. The aspheric terms for surfaces 1, 2, and 3 are tabulated in FIG. 2.

[0017] The light reflected from surface 3 reaches surface 4 where, when in the mirror state, surface 4 gives the light a final reflection toward the image plane 10. The aperture diameter for surface 4 can be 40 mm, and its ROC can be 135.11 mm. In some cases, a cover plate 5 is required for electrode attachment and mechanical stability of the switchable layer 4. This cover plate can be made from N-BK7 material to be transparent in the band of interest and can, as is the case here, have a different front curvature (120.39 mm) than that of layer 4. The back curvature of 5 is in contact with 4 and should therefore have the same curvature as the switchable layer. The cover glass 9 is included as a protection to the sensor array placed at the image plane 10 and can also be made from N-BK7. Windows 6 and 8 help to seal the mirrored surfaces of the annular folded optics against environmental damage, since the surfaces are otherwise open, with no intervening solid between them. These windows can be made from ZnS.

[0018] Upon switching surface 4 to the clear state, an alternate path for the light to travel is opened, as is illustrated in FIG. 3. FIG. 4 is a table of the raytrace parameters for the imager with the wide FOV path shown in FIG. 3. Light from a distant object enters this path through the aperture stop 11, which can have a diameter of 23.6 mm. The light is first refracted by lens 12, which can be a meniscus lens made from ZnSe material, with front ROC of 19.65 mm and aperture diameter of 25.6 mm and back ROC of 25.44 mm and aperture diameter of 33.3 mm. The light refracted from 12 then enters a doublet element composed of lenses 13 and 14. Lens 13 can be made from Schott IGX-A material, with front ROC of 56.08 mm and aperture diameter of 36.5 mm and back ROC of 20.34 mm and aperture diameter of 33 mm. The front surface of lens 14 matches the back surface of 13 in both ROC and aperture, and a suitable adhesive layer that is transparent for SWIR is used to glue the lenses together. Lens 14 can be made from ClearTran material, with back ROC of 412.35 mm and aperture diameter of 32.7 mm. Light refracted through this doublet enters the aperture of lens 15, which can be made from ClearTran material. The front ROC of 15 can be 30.71 mm and aperture diameter of 32.5 mm and back ROC of 37.29 mm and aperture diameter of 36.9 mm. Lens 15 additionally has an aspheric departure from the sphere on the back surface, as indicated by the parameters in FIG. 4. Light refracted by lens 15 enters the aperture of lens 16, which can be made from ClearTran material, with a flat front surface, having infinite ROC and a curved back surface with an ROC of 135.11 mm. Both front and back apertures of lens 16 can be 40 mm. The back surface of lens 16 is the substrate onto which the switchable layer 4 is mounted. When layer 4 is switched to the clear state, the light will pass through 4 and proceed to the image plane 10, passing through elements 5, 8, and 9, in a similar manner as described above for the narrow FOV.

[0019] The effective f/number is an important factor that determines how much light will reach the image plane 10. Annular optics, as are used in the narrow FOV described above, have a central obscuration along the annular axis that reduces the amount of light that would otherwise reach the image plane if the full aperture were used. The effective f/number is calculated by the following formula:

[00002]$f/{\mathrm{number}}_{\mathrm{eff}}=f/{\mathrm{number}\left[1-{\left(\frac{D_{\mathrm{obs}}}{D}\right)}^2\right]}^{-1/2},$

[0020] where D.sub.obs is the diameter of the obscuration, namely the inner diameter of the aperture stop 7, and D is the entrance pupil diameter, namely the outer diameter of 7. When there is no obscuration, D.sub.obs equals 0, and the effective f/number is equal to the full aperture f/number. The subject invention is designed to keep the effective f/number of the narrow FOV equal to that of the wide FOV, which has a value of 1.4. The two fields of view vary in focal length by a factor of three.

[0021] The FOV that is seen at the image plane 10 is controlled by the state of the switchable layer 4. This layer can be created from a switchable material (for example, liquid crystals or electrochromic materials) that is designed to switch between mirror and clear states, as controlled by an electrical voltage signal. FIGS. 5 and 6 show a close-up view of the switchable layer 4, applied to lens 16 and protected by cover glass 5. Electrical connections for applying voltage to layer 4 are provided by wires 17. FIG. 5 demonstrates the mirror state, where the dashed line represents a light ray that follows the narrow FOV path through the annular reflective optics. At surface 4, the mirror state reflects the light towards the image plane 10. The dotted line represents a light ray that comes through the wide FOV refractive path, but is reflected at 4, thus preventing it from arriving at the image plane 10. FIG. 6 demonstrates the clear state, where the dashed line, representing a light ray coming through the annular reflective optics, transmits through surface 4 and does not progress toward the image plane 10. With surface 4 in the clear state, the dotted line, representing a light ray coming through the wide FOV refractive path, transmits through 4 and is directed toward the image plane.

[0022] It is obvious that many modifications and variations of the present invention are possible in light of the above teachings. It is therefore to be understood that within the scope of the appended claims, the invention may be practiced otherwise than as described.