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Only-readable three-dimensional optical storage device

  • US 6,738,337 B2
  • Filed: 06/08/2001
  • Issued: 05/18/2004
  • Est. Priority Date: 07/20/2000
  • Status: Expired due to Fees
First Claim
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1. A only-readable three-dimensional optical storage, wherein said storage consists of two systems:

  • A writing system which includes a computer, a beam splitter, a precise rotary table, a writing light source, lenses, a spatial light modulator, a spatial filter, mirrors, a photorefractive crystal and a CCD; and

    in which said spatial light modulator (104), precise rotary table (109), CCD (111) are connected to said computer (112);

    said photorefractive crystal (107) is fixed on said precise rotary table (109);

    said beam splitter (101) is placed in the front of said writing light source (100), and said spatial filter (102), lens (103), spatial light modulator (104) is placed in turn between said beam splitter (101) and said mirror (105);

    said mirror (108) is placed between said beam splitter (101) and said photorefractive crystal (107);

    said lens (106) is placed between said beam splitter (101) and said photorefractive crystal (107); and

    said lens (110) and said CCD (111) is in turn placed behind said photorefractive crystal (107) and opposite to the lens (106), with a intersect angle 2θ

    of two writing beam from the lens (106) and mirror (108) being within the range of 10°

    ˜

    35°

    ;

    a read-out system which includes a computer, a precise rotary table, a slit, a phase-mismatch adjustor, a readout light source, a photorefractive crystal, lenses and a CCD;

    in which said precise rotary table (203) and CCD (205) are connected to said computer (206);

    said photorefractive crystal (204) is fixed on said precise rotary table (203), and said slit (201), phase-mismatch adjustor (202), precise rotary table (203), photorefractive crystal (204), lens (207) and CCD (205) are in turn placed behind the readout light source (200), with a angle (180°

    -2α

    ) between the light from the phase-mismatch adjustor (202) and the diffracted light to the lens (207) being a function of θ

    as λ

    wsinθ



    rsinα

    .

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