The present invention relates generally to optical devices, and more particularly to an optical sensor utilizing background reconstruction image processing techniques in order to provide a much higher level of resolution of a localized object within a background scene.
Optical sensors are devices which for decades have been used to detect and record optical images. Various types of optical sensors have been developed which work in the Ultra Violet Bands, Infra Red Bands as well as in the Visible Bands of operation. Examples of such devices include Weather Sensors, Terrain Mapping Sensors, Surveillance Sensors, Medical Probes, Telescopes and Television Cameras.
An optical sensor typically includes an optical system and one or more detectors. The optical system portion is made up of various combinations of lenses, mirrors and filters used to focus light onto a focal plane located at the image plane of the optical system. The detectors which make up the image plane are used to convert the light received from the optical system into electrical signals. Some types of optical sensors use film rather than detectors to record the images. In this case, the grain size of the film is analogous to the detectors described above
An important performance characteristic of optical sensors is their xe2x80x9cspatial resolutionxe2x80x9d which is the size of the smallest object that can be resolved in the image or, equivalently, the ability to differentiate between closely spaced objects. If the optical system is free from optical aberrations (which means is being xe2x80x9cwell correctedxe2x80x9d) the spatial resolution is ultimately limited by either diffraction effects or the size of the detector.
Diffraction is a well known characteristic of light which describes how light passes through an aperture of an optical system. Diffraction causes the light passing through an aperture to spread out so that the point light sources of a scene end up as a pattern of light (known as a diffraction pattern) diffused across the image. For a well corrected, unobscured optical system known as a diffraction limited system, the diffraction pattern includes a very bright central spot, surrounded by somewhat fainter bright and dark rings which gradually fade away as the distance from the central spot increases.
An optical sensor that is designed to be diffraction limited usually has a very well corrected optical system and detectors sized so that the central spot of the diffraction pattern just fits within the active area of the detector. With conventional sensors, making the detectors smaller does not improve resolution and considerably increases the cost due to the expense of the extra detectors and the associated electronics.
The size of the aperture used in the optical system determines the amount of resolution lost to diffraction effects. In applications such as camera lenses and telescope objectives, the aperture size is normally expressed as an f-number which is the ratio of the effective focal length to the size of the clear aperture. In applications such as microscope objectives, the aperture size is normally expressed as a Numerical aperture (NA) which is the index of refraction times the sine of the half angle of the cone of illumination. For a given focal length, a high f-number corresponds to a smaller aperture, while a higher Numerical aperture corresponds to a larger aperture.
A basic limitation of conventional optical sensors is the aperture size required for a given level of resolution. Higher resolution images require larger apertures. In many situations the use of such a system is very costly. This is because using a larger aperture requires a significantly larger optical system. The cost for larger systems which have apertures with diameters greater than one foot is typically proportional to the diameter of the aperture raised to a power of xe2x80x9cxxe2x80x9d. The variable xe2x80x9cxxe2x80x9d usually ranges from 2.1 to 2.9 depending on a number of other particulars associated with the sensor such as its wave band, field of regard, and field of view.
The size of the optical sensor is particularly relevant for systems that fly on some type of platform, either in space or in the air. Under such conditions the sensor must be light weight, strong, and capable of surviving the rigors of the flight environment. Thus the cost of going to a larger optical system can be in the hundreds of millions of dollars for some of the larger and more sophisticated sensors. Practical considerations, such as the amount of weight the host rocket, plane, balloon, or other vehicle can accommodate, or the amount of space available, may also limit the size of the sensor. These practical considerations can prevent a larger system from being implemented no matter how large the budget.
A number of optical imaging techniques have been developed to increase spatial resolution One such technique is known as sub-pixel resolution. In sub-pixel resolution the optical system is limited in spatial resolution not by diffraction but by the size of the detectors or pixels. In this case, the diffraction pattern of the aperture is much smaller than the detectors, so the detectors do not record all the resolution inherent in the optical system""s image. Sub-pixel resolution attempts to reconstruct an image that includes the higher resolution not recorded by the detectors. This technique does not require hardware or system operation changes in order to work. Examples of sub-pixel resolution techniques are disclosed in an article in ADVANCED SIGNAL PROCESSING ALGORITHMS, ARCHITECTURES AND IMPLEMENTATIONS II, by J. B. Abbiss et al., The International Society For Optical Engineering, Volume 1566, P. 365 (1991).
Another example is the use of xe2x80x9cthinned aperturexe2x80x9d systems where for example, a widely-spaced pattern of small holes is used as a substitute for the complete aperture. However, even xe2x80x9cthinned a perturesxe2x80x9d are limited in resolution by diffraction theory and by the outer diameter of the widely-spaced pattern of small holes. Note that current electro-optical systems are sometimes designed so that the size of their detector matches the size of the diffraction blur of their optics.
Other examples of optical imaging techniques are disclosed in an article entitled SUPER RESOLUTION ALGORITHMS FOR A MODIFIED HOPFIELD NEURAL NETWORK, by J. B. Abbiss et al., IEEE Transactions On Signal Processing, Vol. 39, No. 7, July 1991 and in a paper entitled FAST REGULARIZED DECONVOLUTION IN OPTICS AND RADARS, by J. B. Abbiss et al., presented at the 3rd IMA Conference on Mathematics in Signal Processing. These techniques use linear algebra and matrix techniques to restore signals or images from a limited discrete data set.
The previously described techniques have a number of drawbacks with regard to optical sensors. First, only one of these techniques is directed toward a diffraction limited device. In addition, these techniques often produce systems of equations which cannot be solved due to the practical constraints on computing power. Furthermore, none of the previously described techniques specify either the types of detectors or other system parameters which are used along with these techniques.
It is, therefore, an object of the present invention to provide a technique for optimally increasing the resolution of an optical sensor that is diffraction limited (using super-resolution techniques) without using a substantially larger aperture.
The invention provides a method of improving the spatial resolution of an object using a background reconstruction approach wherein a localized object containing high spatial frequencies is assumed to exist inside a background scene containing primarily low and/or very high spatial frequencies compared to the spatial frequencies of the localized object. The imaging system cannot pass these high spatial frequencies (neither the high frequencies of the object, nor the very high frequencies of the background). The background image""s low spatial frequencies are used to reconstruct the background scene in which the localized object is situated. Using this reconstructed background and the space limited nature of the localized object (i.e. it is only present in part of the scene, not the entire scene), the high spatial frequencies that did not pass through the optical system are restored, reconstructing a detailed image of the localized object.
The improvement comprises filtering the noisy blurred background data of the same scene to obtain noise suppressed data; applying estimations of point spread functions associated with the noise suppressed data and optical system to estimates of the noise suppressed data to obtain a reconstructed background image (Ir(X)); and low pass filtering the noisy blurred scene data containing the object to be reconstructed (D1) and using the reconstructed background image (Ir(x)) to eliminate the background data from the image data to obtain a reconstructed image of an object with increased spatial resolution.
USPTO Backgrounds
USPTO Backgrounds