Collimating waveguide apparatus and method

• US 8,534,901 B2
• Filed: 09/13/2010
• Issued: 09/17/2013
• Est. Priority Date: 09/13/2010
• Status: Active Grant

• Current Assignee: Seoul Semiconductor Co., Ltd.
• Original Assignee: Teledyne Reynolds, Inc. (Teledyne Technologies Incorporated)
• Inventors: Panagotacos, George W., Pelka, David G., Unger, Blair L
• Primary Examiner(s): Makiya, David J
• Assistant Examiner(s): Gyllstrom, Bryon T
• Application Number:
  US12/880,876
• Publication Number:
  US 20120063166A1
• Time in Patent Office: 1,100 Days
• Field of Search: 362/615, 362623-626, 362/628, 362559-561
• US Class Current: 362/625
• CPC Class Codes: G02B 6/0016 Grooves, prisms, gratings, scattering particles or rough surfaces
• CPC Class Codes: G02B 6/002 by shaping at least a portion of the light guide, e.g. with collimating, focussing or diverging surfaces
• CPC Class Codes: G02B 6/0038 Linear indentations or grooves, e.g. arc-shaped grooves or meandering grooves, extending over the full length or width of the light guide
• CPC Class Codes: G02B 6/0045 by shaping at least a portion of the light guide
• CPC Class Codes: G02B 6/0046 Tapered light guide, e.g. wedge-shaped light guide

Abstract

A collimating waveguide, an optical backlight apparatus, and a method of producing a collimated beam of radiant electromagnetic energy are disclosed. A collimating waveguide comprises an input surface to receive radiant electromagnetic energy from a point source and an output surface to emit an output beam of substantially collimated radiant electromagnetic energy. A first collimating surface of the waveguide receives a beam of the radiant electromagnetic energy entering from the input surface traveling in a first direction and reflects the radiant electromagnetic energy into a substantially collimated beam of radiant electromagnetic energy traveling in a second direction, which is the reverse of the first direction. A second collimating surface of the waveguide receives the substantially collimated beam of radiant electromagnetic energy and to redirect the substantially collimated beam toward the output surface. An optical backlight apparatus comprises a reflective cavity to receive the collimating waveguide and a diffuser located over the output surface of the collimating waveguide.

Claims

1. A collimating waveguide, comprising:

an input surface comprising a microstructure to receive radiant electromagnetic energy from a point source, wherein the microstructure comprises a plurality of linear prisms each one defining an apex angle, a convex portion defining a radius, and a concave portion defining a radius, wherein the radius of the convex portion is greater than the radius of the concave portion;

an output surface to emit an output beam of substantially collimated radiant electromagnetic energy;

a first collimating surface to receive a beam of the radiant electromagnetic energy entering from the input surface traveling in a first direction and to reflect the radiant electromagnetic energy into a substantially collimated beam of radiant electromagnetic energy traveling in a second direction, which is the reverse of the first direction, wherein the first collimating surface comprises a curved surface, wherein the curved surface is defined by a first radius of curvature R₁ about a first axis and a second radius of curvature R₂ about a second axis, wherein the first and second axes are orthogonal; and

a second collimating surface to receive the substantially collimated beam of radiant electromagnetic energy and to redirect the substantially collimated beam toward the output surface.

2. The collimating waveguide of claim 1, wherein the apex angle is about 80°

, the radius of the convex portion is about 50 μ

m, and the radius of the concave portion is about 10 μ

m and wherein the plurality of linear prisms are spaced apart by a distance of about 0.1 mm.

3. The collimating waveguide of claim 1, wherein the microstructure of the input surface comprises an optically active input area of about 1.4 mm by about 3 mm.

4. The collimating waveguide of claim 1, wherein the output surface is substantially optically flat to minimize surface roughness.

5. The collimating waveguide of claim 1, wherein the output surface is a smooth total internal reflection (TIR) surface.

6. The collimating waveguide of claim 1, wherein the output surface has an aspect ratio of about 4:

3.

7. The collimating waveguide of claim 6, wherein the output surface has an optically active area of about 15 mm by about 20 mm.

8. The collimating waveguide of claim 1, wherein the output surface has an aspect ratio of about 16:

9.

9. The collimating waveguide of claim 1, wherein the curved surface is a spherical surface, wherein the first radius of curvature R₁ is equal to the second radius of curvature R₂.

10. The collimating waveguide of claim 9, wherein the spherical surface comprises a radius of curvature R₁=R₂ of about 55 mm.

11. The collimating waveguide of claim 1, wherein the second collimating surface comprises a microstructure.

12. The collimating waveguide of claim 11, wherein the microstructure comprises a plurality of linear prisms each one defining a plurality of prismatic features having a predetermined spacing to optimize the uniformity of the radiant electromagnetic energy redirected to the output surface, wherein each prismatic feature comprises a first facet and a second facet.

13. The collimating waveguide of claim 12, wherein the first facet forms a first angle relative to an axis substantially parallel to the output surface and the second facet forms a second angle relative to the axis, and wherein the first angle is less than the second angle.

14. The collimating waveguide of claim 13, wherein the spacing of the prismatic features is about 0.1 mm, the first angle is about 10°

, and the second angle is about 37.5°

.

15. The collimating waveguide of claim 1, wherein the first and second collimating surfaces are optically reflective surfaces.

16. The collimating waveguide of claim 15, wherein the optically reflective surfaces are made of a metallic material.

17. The collimating waveguide of claim 16, wherein the metallic material comprises aluminum.

18. The collimating waveguide of claim 1, wherein the output beam of substantially collimated radiant electromagnetic energy emitted from the output surface is substantially normal to the output surface.

19. The collimating waveguide of claim 1, wherein the input surface microstructure is to diverge the radiant electromagnetic energy received from the point source so as to uniformly fill an aperture defined by the first collimating surface with the radiant electromagnetic energy.

20. A collimating optical backlight, comprising:

a reflective cavity; and

a collimating waveguide located with the reflective cavity, wherein the collimating waveguide comprises;

an input surface comprising a microstructure to receive radiant electromagnetic energy from a point source, wherein the microstructure comprises a plurality of linear prisms each one defining an apex angle, a convex portion defining a radius, and a concave portion defining a radius, wherein the radius of the convex portion is greater than the radius of the concave portion;

an output surface to emit an output beam of substantially collimated radiant electromagnetic energy;

a first collimating surface to receive a beam of the radiant electromagnetic energy entering from the input surface traveling in a first direction and to reflect the radiant electromagnetic energy into a substantially collimated beam of radiant electromagnetic energy traveling in a second direction, which is the reverse of the first direction, wherein the first collimating surface comprises a curved surface, wherein the curved surface is defined by a first radius of curvature R₁ about a first axis and a second radius of curvature R₂ about a second axis, wherein the first and second axes are orthogonal; and

a second collimating surface to receive the substantially collimated beam of radiant electromagnetic energy and to redirect the substantially collimated beam toward the output surface.

21. The collimating optical backlight of claim 20, further comprising a source of radiant electromagnetic energy coupled to the input surface of the collimating waveguide.

22. The collimating optical backlight of claim 21, wherein the source of radiant electromagnetic energy is a light emitting diode (LED).

23. The collimating optical backlight of claim 20, comprising a diffuser located over the output surface of the collimating waveguide.

24. The collimating optical backlight of claim 23, wherein the diffuser comprises a holographic pattern.

25. The collimating optical backlight of claim 23, wherein the diffuser comprises a thin film micro-lens array.

26. The collimating optical backlight of claim 23, wherein the diffuser redirects the radiant electromagnetic energy from the output surface of the collimating waveguide to a narrow collimated and uniform angular field of view.

27. The collimating optical backlight of claim 26, wherein the angular field of view is about 10°

.

28. The collimating optical backlight of claim 20, wherein the reflective cavity comprises a high efficiency white diffuse reflective material.

29. The collimating optical backlight of claim 20, wherein the input surface microstructure is to diverge the radiant electromagnetic energy received from the point source so as to uniformly fill an aperture defined by the first collimating surface with the radiant electromagnetic energy.

30. A method of producing a collimated beam of radiant electromagnetic energy, the method comprising:

optically coupling radiant electromagnetic energy from a point source into an input surface comprising a microstructure, wherein the microstructure comprises a plurality of linear prisms each one defining an apex angle, a convex portion defining a radius, and a concave portion defining a radius, wherein the radius of the convex portion is greater than the radius of the concave portion;

transmitting the radiant electromagnetic energy from the input surface to a first collimating surface in a first direction by reflection and total internal reflection (TIR);

reflecting the radiant electromagnetic energy by the first collimating surface into a substantially collimated beam of radiant electromagnetic energy traveling in a second direction, which is the reverse of the first direction, wherein the first collimating surface comprises a curved surface, wherein the curved surface is defined by a first radius of curvature R₁ about a first axis and a second radius of curvature R₂ about a second axis, wherein the first and second axes are orthogonal;

redirecting the substantially collimated beam of radiant electromagnetic energy by a second collimating surface into a substantially collimated beam toward an output surface; and

emitting the substantially collimated beam of electromagnetic energy from the output surface.

31. The method of claim 30, comprising reflecting the optically coupled radiant electromagnetic energy by an internal surface of the output surface by total internal reflection (TIR).

32. The method of claim 30, wherein redirecting the substantially collimated beam of radiant electromagnetic energy by the second collimating surface comprising reflecting the substantially collimated beam of radiant electromagnetic energy by a plurality of linear prisms each one defining a plurality of prismatic features having a predetermined spacing to optimize the uniformity of the radiant electromagnetic energy redirected to the output surface, wherein each prismatic feature comprises a first facet and a second facet.

33. The method of claim 30, wherein emitting an output beam of substantially collimated radiant electromagnetic energy from the output surface, comprises emitting an output beam of substantially collimated radiant electromagnetic energy from the output surface at a substantially normal angle relative to the output surface.

34. The method of claim 30, comprising diverging by the input surface microstructure the radiant electromagnetic energy received from the point source and uniformly filling an aperture defined by the first collimating surface with the radiant electromagnetic energy.