A proposed joint-transform optical correlator (JTOC) would be capable of operating as a real-time pattern-recognition processor. The key correlation-filter reading/writing medium of this JTOC would be an updateable holographic photopolymer. The high-resolution, high-speed characteristics of this photopolymer would enable pattern-recognition processing to occur at a speed three orders of magnitude greater than that of state-of-the-art digital pattern-recognition processors. There are many potential applications in biometric personal identification (e.g., using images of fingerprints and faces) and nondestructive industrial inspection.

Conventional and Proposed JTOCs differ in geometry and in the media (CCD versus holographic photopolymer) used to record holograms.
In order to appreciate the advantages of the proposed JTOC, it is necessary to understand the principle of operation of a conventional JTOC. In a conventional JTOC (shown in the upper part of the figure), a collimated laser beam passes through two side-by-side spatial light modulators (SLMs). One SLM displays a real-time input image to be recognized. The other SLM displays a reference image from a digital memory. A Fourier-transform lens is placed at its focal distance from the SLM plane, and a charge-coupled device (CCD) image detector is placed at the back focal plane of the lens for use as a square-law recorder.

Processing takes place in two stages. In the first stage, the CCD records the interference pattern between the Fourier transforms of the input and reference images, and the pattern is then digitized and saved in a buffer memory. In the second stage, the reference SLM is turned off and the interference pattern is fed back to the input SLM. The interference pattern thus becomes Fourier-transformed, yielding at the CCD an image representing the joint-transform correlation between the input and reference images. This image contains a sharp correlation peak when the input and reference images are matched.

The drawbacks of a conventional JTOC are the following:

  • The CCD has low spatial resolution and is not an ideal square-law detector for the purpose of holographic recording of interference fringes. A typical state-of-the-art CCD has a pixel-pitch limited resolution of about 100 lines/mm. In contrast, the holographic photopolymer to be used in the proposed JTOC offers a resolution > 2,000 lines/mm. In addition to being disadvantageous in itself, the low resolution of the CCD causes overlap of a DC term and the desired correlation term in the output image. This overlap severely limits the correlation signal-to-noise ratio.
  • The two-stage nature of the process limits the achievable throughput rate. A further limit is imposed by the low frame rate (typical video rates) of low- and medium-cost commercial CCDs.

In the proposed JTOC, shown in the lower part of the figure, a collimated beam (denoted the writing beam) from a diode laser would first be split into two orthogonal parts that would then be reflected at oblique angles. As in the conventional JTOC, one part of the beam would illuminate an input SLM while the other part would illuminate a reference SLM. In this case, however, there would be two Fourier-transform lenses: one for the input image and one for the reference image. The input and reference beams would intersect at the center of the Fourier-transform plane. A holographic photopolymer film would be placed in this plane for recording the interference fringes.

A second diode laser would generate a readout light beam incoherent with the writing beam (optionally at approximately the same or a different wavelength). The readout beam would illuminate the holographic photopolymer film from the side opposite that of the writing beam. A thin-film beam splitter would be placed between the input Fourier-transform lens and the photopolymer film to intercept the readout beam as modified by passage through the photopolymer film. The modified readout beam would be reflected by this beam splitter, then a third Fourier-transform lens would focus this beam to a correlation output image on a complementary metal oxide/semiconductor (CMOS) photodetector array. When the input scene contained a target image matching the reference image, a sharp correlation peak would appear at the location of the centroid of the input image.

The high-speed-recording and low-data-retention-time characteristics of the photopolymer would make it possible to record holograms in real time repeatedly by use of pulsing of the writing laser in synchronism with updating of the images on the SLMs, while reading out the correlation image continuously by use of continuous operation or synchronous pulsing of the readout laser. The off-axis nature of the holographic-recording geometry of the proposed JTOC would confer an additional advantage that is not intuitively obvious but can be discerned by examination of the equations describing the holographic process: The geometry would give rise to a spatial separation of cross-correlation and convolution components of the output image, such that, as desired, the CMOS photodetector array would retrieve only the correlation component.

This work was done by Tien-Hsin Chao and Kevin Cammack of Caltech for NASA’s Jet Propulsion Laboratory.

In accordance with Public Law 96-517, the contractor has elected to retain title to this invention. Inquiries concerning rights for its commercial use should be addressed to:

Innovative Technology Assets Management
JPL
Mail Stop 202-233
4800 Oak Grove Drive
Pasadena, CA 91109-8099
(818) 354-2240
E-mail: This email address is being protected from spambots. You need JavaScript enabled to view it.

Refer to NPO-40994.


This Brief includes a Technical Support Package (TSP).
Pattern-Recognition Processor Using Holographic Photopolymer

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This article first appeared in the March, 2006 issue of Photonics Tech Briefs Magazine.

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