Liquid crystal matrices

• US 4,278,327 A
• Filed: 11/26/1979
• Issued: 07/14/1981
• Est. Priority Date: 11/26/1979
• Status: Expired due to Term

• Current Assignee: Sperry Corporation (Unisys Corporation)
• Original Assignee: Sperry Corporation (Unisys Corporation)
• Inventors: Soref, Richard A., McMahon, Donald H.
• Primary Examiner(s): Bauer, Edward S.
• Application Number:
  US06/097,294
• Time in Patent Office: 596 Days
• Field of Search: 350/347 V, 350/347 R, 350/334, 350/96.13, 350/96.14
• US Class Current: 349/197
• CPC Class Codes: G02F 1/1326 Liquid crystal optical waveguides or liquid crystal cells specially adapted for gating or modulating between optical waveguides
• CPC Class Codes: G02F 1/1393 the birefringence of the liquid crystal being electrically controlled, e.g. ECB-, DAP-, HAN-, PI-LC cells G02F1/1396, G02F1/141 take precedence
• CPC Class Codes: G02F 1/315 based on the use of controlled internal reflection

Abstract

The improved electrooptical devices provide means for switching pluralities of polarized or unpolarized optical signals between input and output multimode single strand light guides. The electrooptical switching elements employ electric field-effect liquid crystal compositions and are adapted to use in the construction of large scale, integrated multiple switching arrays.

Claims

1. An optical switching matrix comprising:

first port means for propagating an input light beam having components in first and second linearly polarized states so as to intersect, at a predetermined angle and at a first location, a confined layer of electrooptically active nematic material for reflection of said first polarized state component and for transmission therethrough of said second polarized state component for forming respective second and third divergent light beams,

polarization converter means for interchanging the respective polarizations of said respective second and third divergent light beams, and

reflector means for redirecting said second and third light beams so as to intersect, at said predetermined angle and at a second location, said confined layer for redirecting said second and third light beams to form a combined light beam, said combined light beam propagating through second port means in substantially the same direction as said input light beam.

2. Apparatus as described in claim 1 wherein said polarization converter means is disposed between said first port means and said reflector means.

3. Apparatus as described in claim 1 wherein said polarization converter means is disposed at said reflector means in contiguous relation therewith.

4. Apparatus as described in claim 3 wherein said layer of electrooptically active nematic material is confined between first and second spaced-apart transparent bodies having respective opposed first and second parallel surfaces at said layer.

5. Apparatus as described in claim 4 wherein each of said spaced-apart transparent bodies has first and second transparent end faces disposed at said acute angle with respect to said first or second parallel surfaces.

6. Apparatus as described in claim 5 wherein said acute angle is selected from an operative range of angles greater than the critical angle θ

_c of total internal reflection of the material of said transparent body.

7. Apparatus as described in claim 5 wherein said acute angle lies substantially between θ

_c +1° and

θ

_c +7°

, where θ

_c is the critical angle of internal reflection of the material of said transparent body.

8. Apparatus as described in claim 5 wherein said acute angle is substantially θ

_c +2°

, where θ

_c is the critical angle of internal reflection of the material of said transparent body.

9. Apparatus as described in claim 5 wherein each said transparent body includes six planar sides, two sides taking the form of substantially parallel trapezoids each having only two equal sides.

10. Apparatus as described in claim 5 wherein said first and second port means are affixed in perpendicular abutted relation respectively to selected ones of said respective end faces.

11. Apparatus as described in claim 10 wherein said transparent bodies each include an outer surface parallel to said first and second surfaces adapted to serve as said reflector means.

12. Apparatus as described in claim 11 wherein said respective reflector means are mounted centrally upon said respective first and second outer surfaces in parallel relation thereto.

13. Apparatus as described in claim 12 wherein said polarization converter means is disposed between each said reflector means and said respective first and second surfaces.

14. Apparatus as described in claim 5 wherein said polarization converter means are disposed within said transparent body means at said acute angle to said first and second parallel surfaces.

15. Apparatus as described in claim 5 wherein said polarization converter means are disposed within said transparent body means at right angles to said first or second parallel surfaces.

16. Apparatus as described in claim 1 further including unitary means for imposing an electric field simultaneously across said confined layer of electrooptically active nematic material at said first and second locations.

17. Apparatus as described in claim 16 wherein said layer of electrooptically active nematic material is characterized by orientation of the long axes of the molecules thereof parallel to said layer and in a direction parallel to the optical incidence plane in the absence of an enabling electric field thereacross.

18. Apparatus as described in claim 1 further including means for selectively imposing discrete electric fields across said confined layer of electrooptically active nematic material at said first and second locations.

19. Apparatus as described in claim 18 wherein:

said means for selectively imposing electric fields at said first and second locations comprises transparent first and second pairs of transparent electrodes, and

said polarization converter means comprises half-wave plate substrate means in contiguous relation with one of the electrodes of each of said first and second pairs of transparent electrodes.

20. Apparatus as described in claim 19 wherein said layer of electrooptically active nematic material is characterized by orientation of the long axes of the molecules thereof parallel to said layer in a direction parallel to the optical incidence plane in the absence of enabling electric fields at said first and second electric fields.

21. An optical switching matrix comprising:

at least first and second transparent prismatic bodies,

first port means affixed to one of said bodies for propagating an input light beam having components in first and second lineally polarized states so as to intersect, at a predetermined angle and at a first location, a layer of electrooptically active nematic material confined between parallel disposed spaced sides of said first and second transparent prismatic bodies for reflection of said first polarized state component and for transmission therethrough of said second polarized state component for forming respective second and third divergent light beams, the spatial splitting of said second and third beams occurring in the absence of an enabling electric field at said first location,

reflector means for redirecting said second and third light beams so as to intersect, at said predetermined angle and at a second location, said confined layer for redirecting said second and third light beams to form a combined light beam with the structure of said optical switching matrix being so configured that the respective polarization states of said respective second and third divergent beams remain unchanged before recombination thereof,

second port means affixed to the first of said bodies for the output propagation of said combined light beam when an enabling electric field is absent at said second location, the light flow in the second port being substantially at 46°

to said input light beam, and

third port means affixed to the second of said bodies for the output propagation of said combined light beam when an enabling electric field is present at said second location, the light flow in said third port being in the same direction as said input beam.

22. Apparatus as described in claim 21 further including means for selectively imposing an electric field across said confined layer of electrooptically active nematic material only at said second location.

23. Apparatus as described in claim 21 wherein said means for selectively imposing an electric field at said second location comprises opposed transparent electrodes respectively affixed to said first and second transparent prismatic bodies at said second location remote from said first location.

24. Apparatus as described in claim 23 wherein said layer of electrooptically active nematic material is characterized by orientation of the long molecular axes thereof parallel to the plane of said layer in a direction perpendicular to the optical incidence plane in the absence of an enabling electric field at said second location.

25. Apparatus as described in claim 23 wherein said layer of electrooptically nematic material is characterized by orientation of the long molecular axes thereof perpendicular to the plane of said layer in the presence of an enabling electric field at said second location.

26. An optical switching matrix comprising,

first, second and third transparent prismatic bodies in spaced apart relation for defining first and second electroactive regions,

first and second electrooptically active layer means respectively disposed in contiguous first and second locations within said first electroactive region,

third and fourth electrooptically active means disposed in respective spaced apart third and fourth locations within said second electroactive region,

electrooptically inactive means disposed between said third and fourth locations,

said first, second, third, and fourth electrooptically active layer means including electrooptically active nematic material selectively activatable by associated electric fields at said respective first, second, third, or fourth locations and cooperating with said electrooptically inactive means for selectively transmitting light incident at a predetermined angle at said first or third location therethrough or for reflecting same.

27. Apparatus as described in claim 26 further including:

input light port means affixed one each to each of said bodies for selectively illuminating said first or third electrooptically active layer means, and

output light port means affixed one each to each of said bodies opposite said input light port means for receiving light selectively reflected at least from or transmitted through said second or fourth electrooptically active layer means.

28. Apparatus as described in claim 27 wherein:

said first and third transparent prismatic bodies have respective outer surfaces respectively opposite said first and second electroactive regions,

first reflector means at said outer surface of said first transparent prismatic body for directing incident light into said second optically active layer means, and

second reflector means at said outer surface of said transparent prismatic body for directing light into said electrooptically inactive means or into said fourth optically active layer means.

29. Apparatus as described in claim 28 wherein said first, second, third, and fourth electrooptically active means comprise the same nematic material and the molecular long axes thereof lie parallel to the respective planes of said electrooptically active means in a direction perpendicular to the optical incidence plane in the absence of enabling electric fields.

30. Apparatus as described in claim 29 wherein the optical index of said electrooptically inactive means matches that of said first, second, third, and fourth transparent prismatic bodies.

31. Apparatus as described in claim 26 wherein:

each of said first, second, and third transparent prismatic bodies is characterized by symmetry about a respective plane, and

each of said first, second, and third transparent prismatic bodies is so disposed that said respective planes are aligned whereby said optical switching matrix is characterized by planar geometrical symmetry.

32. An optical switching matrix comprising:

first, second, third, fourth, and fifth transparent prismatic bodies in spaced apart relation for defining therebetween first, second and third electroactive regions,

first and second electrooptically active layer means respectively disposed centrally in contiguous side-by-side relation within said first electroactive region,

first and second electrooptically inactive regions respectively disposed on each side of said first and second electrooptically active layer means and coplanar therewith,

third, fourth, fifth, and sixth electrooptically active layer means respectively disposed in coplanar relation within said second electroactive region, said third electrooptically active layer means being disposed at one end of said second electroactive region, said fourth, fifth, and sixth electrooptically active layer means being disposed in contiguous coplanar relation and spaced apart from said third electrooptically active layer means at a second end of said second electroactive region,

seventh and eighth electrooptically active layer means respectively disposed centrally in contiguous relation within said third electroactive region, and

third and fourth electrooptically inactive regions respectively spaced on each side of said seventh and eighth electrooptically active layer means and coplanar therewith.

33. Apparatus as described in claim 32 wherein:

said first and second electrooptically active layer means is characterized by molecular long axis disposition in a first direction, and

said third, fourth, fifth, sixth, seventh, and eighth electrooptically active layer means are characterized by molecular axis disposition at right angles to said first direction, both in the absence of an enabling electric field.

34. Apparatus as described in claim 32 wherein said first, second, third, fourth, fifth, sixth, seventh, and eighth electrooptically active layer means include optically active nematic material selectively activatable by associated electric fields and cooperating selectively with said first, second, third, and fourth optically inactive means for transmitting light incident at a predetermined angle at said third electrooptically active layer therethrough or for reflecting the same.

35. Apparatus as described in claim 34 further including:

input light port means affixed one each to each of said second and third transparent prismatic bodies for selectively illuminating said third electrooptically active means, and

at least one light output port means affixed one each to each of said bodies opposite said input light port means for receiving light selectively reflected from or transmitted through said first, second, third, fourth, fifth, sixth, seventh, or eighth optically active layer means.

36. Apparatus as described in claim 35 wherein:

said first and fourth transparent prismatic bodies have respective outer surfaces opposite said first and third electroactive regions,

first reflector means at said outer surface of said first transparent prismatic body for directing incident light into said first or second optically active means or into said second electrooptically inactive region, and

second reflector means at said outer surface of said fourth transparent prismatic body for directing light into said seventh or eighth electrooptically active means or into said fourth electrooptically inactive means.

37. Apparatus as described in claim 32 wherein the optical index of said electrooptically inactive means matches that of said first, second, third, and fourth transparent prismatic bodies.

38. Apparatus as described in claim 32 wherein said first, second, third, fourth, fifth, sixth, seventh, and eighth optically active means include positive anisotropy nematic liquid crystal material.

39. Apparatus as described in claim 32 wherein:

each of said first, second, third, and fourth transparent prismatic bodies is characterized by symmetry about a respective plane, and

each of said first, second, third, and fourth transparent prismatic bodies is so disposed that said respective planes are aligned whereby said optical switching matrix displays planar geometrical symmetry.