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Holographic projection screen for displaying a three-dimensional color images and optical display system using the holographic screen

  • US 20010006426A1
  • Filed: 01/25/2001
  • Published: 07/05/2001
  • Est. Priority Date: 07/18/1996
  • Status: Abandoned Application
First Claim
Patent Images

1. An optical display system for displaying stereoscopic or multi-view color images comprising:

  • a holographic screen; and

    two or more image projectors which project the stereoscopic or multi-view color images on said holographic screen, a distance between exit pupils of the two or more image projectors being decided depending on a viewer'"'"'s inter-eye distance, wherein said holographic screen is formed by a method including the steps of;

    (a) placing a photoplate on an x-y plane of a three dimensional space, wherein the center of the photoplate is disposed in the origin of the three dimensional space;

    (b) splitting the laser beam into two beams;

    reference beam and object beam, both beams being used to illuminate the photoplate surface;

    (c) shaping the reference beam as a sperical wave diverging from a point on a z-axis which is located a distance R1 from the photoplate center;

    (d) shaping the object beam so as to illuminate the photoplate through an elongated narrow slit-shaped diffuser inclined to the photoplate surface; and

    (e) recording an interference pattern, which is arising as a result of the superposition of the reference wave with an object wave from the diffuser on the photoplate, whereby the stereoscopic or multiview three dimensional color images is displayed on a recorded screen by the projectors disposed at a distance R3 from the screen, if a viewer'"'"'s eyes are placed at viewing zones which are located behind the screen at a distance R4 the viewing zones being composed of superposed diffuser'"'"'s real images of the different colors, wherein the coordinates of the diffuser point, which is responsible for the contribution of a light with a wavelength X2 in the viewing zone, are calculated from the following equations;

    k2

    r3
    +k1

    (r1-r2)
    =-k2

    r4
    +const
    (1)
    α

    =sin-1

    [k2k1

    sin





    β

    ]
    =sin-1

    [λ

    1
    λ

    2


    sin





    β

    ]
    (2)
    R2=R11+2

    λ

    1


    R1
    λ

    2


    R4
    (3)
    where r1 is the distance between an arbitrary point (x,y) on the photoplate and a position of the source of the reference beam;

    r2 and R2 are the distances between a point (x,y) on the photoplate and a point on the diffuser and between the coordinate origin and the same diffuser point;

    α

    is the angle between R2 straight line and the z-axis;

    r3 is the distance between a point (x,y) on the photoplate and a point source of the projection beam;

    r4 is the distance between a point (x,y) on the photoplate and a viewing zone;

    R4 is the distance between an origin and a viewing zone;

    β

    is the angle between R4 straight line and the z-axis;

    λ

    1 and λ

    2 represent wavelengths of the recording and projecting waves, respectively;

    k1 and k2 are wave numbers of the recording and projecting waves, respectively, wherein the diffuser'"'"'s length and position are calculated using equations (2) and (3) for covering an entire spectral range of a projected image.

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