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Bistable device for reflection display with inverse contrast

  • US 6,795,146 B2
  • Filed: 11/08/2002
  • Issued: 09/21/2004
  • Est. Priority Date: 05/12/2000
  • Status: Expired due to Fees
First Claim
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1. A reflective bistable display device, characterized by the fact that it comprises:

  • a) a liquid crystal material (40) contained between two parallel substrates (30, 50) having electrodes on their facing inside surfaces to apply an electric field to said liquid crystal, at least the front substrate (30) and the front electrode being optically transparent;

    b) alignment layers or treatments on the electrodes to orient the liquid crystal and enable at least two distinct stable or metastable textures to be implemented alternatively in the absence of a field, where one of the textures is either non-twisted, or else twisted at a total angle lying in the range −

    90°

    to +90°

    , and the other possible texture presents additional twist to left or to right through an angle that is essentially an integer multiple of 180°

    ;

    c) the thickness d of the liquid crystal layer (40) being selected in such a manner that the product d·

    Δ

    n is close to λ

    0/4, where λ

    0 is the center wavelength of the working spectrum band of the display and Δ

    n is the birefringence of the liquid crystal for said wavelength;

    d) means designed to apply electrical signals to the liquid crystal enabling it to switch between said two distinct textures and to remain in one or other of them after the field has been removed;

    e) a polarizer (10) associated with the front face of the device, placed inside or outside the device;

    f) a specular or diffusing reflective element (60) placed at the rear face of the liquid crystal, inside or outside the device, enabling light to pass twice through the device and return towards an observer or towards additional optical elements; and

    g) a compensator (20) placed between the polarizer and the reflective element, the compensator presenting an optical delay dc·

    Δ

    nc that is close to λ

    0/4.

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