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METHOD OF FORMING AN OPTICAL ELEMENT OF REDUCED THICKNESS

  • US 3,829,536 A
  • Filed: 04/30/1973
  • Issued: 08/13/1974
  • Est. Priority Date: 04/05/1971
  • Status: Expired due to Term
First Claim
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1. A process for producing a fresnelled optical element from a matrix of discrete elements comprising the steps of:

  • providing a plurality of discrete elongate elements, each element having first and second ends with a plurality of elongate side surfaces therebetween;

    aligning said elongate elements in side-by-side relation with said first ends forming a common surface and said elongate side surfaces of each element in contiguous contacting relation with adjacent elements, said side surfaces permitting relative movement between said elements in the direction of the elongation of said elements and said elongate side surfaces inhibiting relative rotation of said elements about the direction of elongation of said elements;

    holding the elements to prevent relative movement at said side surfacEs in the direction of elongation of said elements, forming a continuous optical surface on the common surface defined by the first ends of said aligned elements;

    releasing said hold on said elements;

    realigning said elements in the direction of elongation of said elements to a second aligned position with the peak of the first common ends of each element being on a common surface, said elements during said realigning being maintained in said side-by-side relation with relative movement occurring at said contiguous contacting elongate side surfaces;

    holding the elements in fixed relative alignment in the second aligned position to form a fresnelled matrix of said continuous optical surface;

    forming optical material over the surface defined by the first common ends of said elements to form a first optical surface complementary to the surface defined by said first common ends of said elements; and

    forming a continuous second optical surface on the surface of said optical material on the optically opposite side of said first surface.

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