U.S. patents available from 1976 to present.
U.S. patent applications available from 2005 to present.

Method and apparatus for improving the signal to noise ratio of an image formed of an object hidden in or behind a semi-opaque random media

Patent 5140463 Issued on August 18, 1992. Estimated Expiration Date: Icon_subject March 8, 2010. Estimated Expiration Date is calculated based on simple USPTO term provisions. It does not account for terminal disclaimers, term adjustments, failure to pay maintenance fees, or other factors which might affect the term of a patent.

Patent References

Collimated radiation apparatus
Patent #: 4203037
Issued on: 05/13/1980
Inventor: Gur ,   et al.

Method of X-ray imaging using slit scanning with controlled target erase
Patent #: 4493096
Issued on: 01/08/1985
Inventor: Rieke

Turbid media viewing system
Patent #: 4707128
Issued on: 11/17/1987
Inventor: Coles

High efficiency fluorescent screen pair for use in low energy X radiation imaging
Patent #: 4710637
Issued on: 12/01/1987
Inventor: Luckey ,   et al.

Anti-scatter grid system Patent #: 4875227
Issued on: 10/17/1989
Inventor: Rossi, et al.

Inventors

Application

No. 489942 filed on 03/08/1990

US Classes:

359/559, Using Fourier transform spatial filtering348/31, BACK SCATTER REDUCTION356/337, BY PARTICLE LIGHT SCATTERING378/154Antiscatter grid

Examiners

Primary: Arnold, Bruce Y.
Assistant: Phan, James

Attorney, Agent or Firm

International Classes

G02B 027/00
G01N 021/00
H04N 007/00
G21K 001/00

Abstract

The quality of image of an object hidden inside a highly scattering semi-opaque disordered medium is improved by using space gate imaging or time gate imaging or space time gate imaging. In space gate imaging, a small segment of the object is illuminated at a time. The scattered light is passed through a spatial noise filter. On the image plane, an aperture is open at the position of the image segment which correspond to the segment of the illuminated object. A full image is obtained by scanning the object segment by segment and simultaneously recording the signal at the corresponding image segment. In time gate imaging, the unscattered (i.e. ballistic) portion of the pulse which contains the information of the image is temporally separated from the other (i.e. scattered) portions which contains the noise using a ultrafast laser pulse and temporal gating devices. The technique is in space-time gate imaging, the two techniques are combined to produce an image with a much higher signal to noise ratio. The time separation between the ballistic and scattered light may be increased by increasing thickness of random medium or by introducing small scatters into the random medium so as to make the medium more random. The signal to noise ratio can also be increased by making the random medium less random (so that there will be less scattered light). In addition, the signal to noise ratio can be increased by introducing an absorbing dye into the medium or by using a wavelength for the light which is in the absorption spectrum of the random medium or by making the medium more ordered (i.e. less random) or by using a pair of parallel polarizers.

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