Nano-structured lens for collimating light from surface emitters

• US 9,851,577 B2
• Filed: 10/02/2015
• Issued: 12/26/2017
• Est. Priority Date: 07/17/2015
• Status: Active Grant

• Current Assignee: DiCon Fiber Optics Incorporated
• Original Assignee: DiCon Fiber Optics Incorporated
• Inventors: Lee, Jeffrey, Lee, Ho-Shang
• Primary Examiner(s): CARIASO, ALAN B
• Application Number:
  US14/873,713
• Publication Number:
  US 20170017091A1
• Time in Patent Office: 816 Days
• Field of Search: 362330
• CPC Class Codes: F21V 5/002 using microoptical elements for redirecting or diffusing light
• CPC Class Codes: G02B 21/06 Means for illuminating specimens
• CPC Class Codes: G02B 27/30 Collimators
• CPC Class Codes: G02B 3/0087 with index gradient

Abstract

A light source for providing light comprises a light emitting layer and a lens comprising a periodic structure therein that is periodic along at least one direction in a plane. The structure includes or is formed from at least two optically transparent materials of different optical indices. The lens is separated from the light emitting layer, and the radiation propagating from the light emitting layer within an angle to a line normal to the plane will be transmitted by the lens to a far field in an index-guided mode. The separation between the light emitting layer and the lens is such that near field radiation propagating from the light emitting layer towards the lens not within said angle to the line will be scattered and redirected by the first lens to the far field to thereby collimate the radiation propagating from the light emitting layer to the far field.

Claims

1. A light source for providing light, comprising:

a light emitting layer; and

a first lens comprising a periodic structure therein that is periodic along at least one direction in a plane, said periodic structure formed from at least two optically transparent materials of different optical indices, wherein said first lens is separated from the light emitting layer, and the radiation propagating from the light emitting layer within an angle to a line normal to the plane will be transmitted by the first lens to a far field in an index-guided mode, the separation between the light emitting layer and the first lens being such that near field radiation propagating from the light emitting layer towards the first lens not within said angle to the line will be scattered and redirected by the first lens to the far field to thereby collimate the radiation propagating from the light emitting layer to the far field.

2. The light source of claim 1, said light source further comprising a second layer between and separating the first lens and the light emitting layer.

3. The light source of claim 2, said light emitting layer having a first optical index value, said second layer having a second optical index value, and said periodic structure including a material having a third optical index value, wherein the first optical index value is greater than the second optical index value, and the second optical index value is greater than the third optical index value.

4. The light source of claim 2, said light emitting layer having a first optical index value, said second layer having a second optical index value, and said periodic structure including a material having a third optical index value, wherein the second optical index value is different from the first and third optical index values by not more than 0.5.

5. The light source of claim 4, said light emitting layer including a compound semiconductor material, wherein said second layer includes nanoparticles with optical index value of not less than 2.

6. The light source of claim 2, said second layer comprising a phosphor material that emits radiation in response to radiation from the light emitting layer.

7. The light source of claim 6, said second layer comprising a silicone gel material that forms a mixture with the phosphor material.

8. The light source of claim 7, said silicone gel material being transparent to radiation from the light emitting layer, so that at least some of the radiation from the light emitting layer not absorbed by the phosphor material passes through the second layer and reaches the far field.

9. The light source of claim 1, said periodic structure comprising a material with a band gap energy that is more than the energy of photons emitted by the light emitting layer.

10. The light source of claim 2, said second layer having a thickness less than 10 times the wavelength of the radiation emitted by the light emitting layer.

11. The light source of claim 1, said light emitting layer including a phosphor material, said light source further comprising a device providing radiation to the phosphor material, causing said phosphor material to emit radiation.

12. The light source of claim 11, said device comprising a lamp or a layer of light emitting material.

13. The light source of claim 1, said periodic structure redirecting radiation within a range of wavelengths including ultraviolet, visible and/or near infrared wavelengths.

14. The light source of claim 1, said periodic structure redirecting radiation having a bandwidth within a range of wavelengths from about 300 nanometers to 2 micrometers.

15. The light source of claim 1, said periodic structure comprising a slab of a first material having dispersed therein a periodic arrangement of a second material, said first and second materials having different optical indices.

16. The light source of claim 15, said second material comprising air or a gel having an optical index lower than that of the first material.

17. The light source of claim 15, said first material comprising silicon, semiconductor materials, liquid crystal materials, metal oxides or polymers.

18. The light source of claim 1, said periodic structure comprising pillars dispersed within air or a gel having an optical index material lower than that of the pillars.

19. The light source of claim 18, said pillars comprising silicon, semiconductor materials, a metal oxide or a polymer.

20. The light source of claim 1, said light emitting layer comprising a semiconductor material with light emitting diodes therein.

21. The light source of claim 1, further comprising a second lens that collimates the radiation that is redirected by the first lens with said periodic structure to the far field.

22. The light source of claim 1, said light emitting layer comprising an array of surface light emitters, said light source comprising an array of lenses, each with a periodic structure therein, each of the lenses of the array of lenses redirecting near field radiation from a corresponding one of the array of surface light emitters, after such radiation tunnels through a medium between the light emitting layer and the first lens, to the far field.

23. The light source of claim 1, said light emitting layer emitting radiation of at least two different wavelengths, said first lens causing scattering of a first one of the at least two wavelengths and insignificant scattering of a second one of the at least two wavelengths, said light source further comprising a second lens with a periodic structure that causes scattering of the second one of the at least two wavelengths and insignificant scattering of the first one of the at least two wavelengths.

24. The light source of claim 23, wherein said first lens and said second lens are placed in a tandem arrangement with respect to the light emitting layer, so that the radiation of the first and second wavelengths passes both lenses and is collimated towards the far field.

25. The light source of claim 24, said light emitting layer emitting radiation of more than two different wavelengths, said light source including more than two lenses placed in a tandem arrangement with respect to the light emitting layer, each of the two lenses placed in a tandem arrangement causing scattering of one of the more than two wavelengths and insignificant scattering of the remaining ones of the more than two wavelengths, so that the radiation of the more than two wavelengths passes each of the two lenses placed in a tandem arrangement and is collimated towards the far field.

26. The light source of claim 1, a first portion of said light emitting layer emitting radiation of a first wavelength, and a second portion of said light emitting layer emitting radiation of a second wavelength, wherein said first lens is located adjacent to the first portion to collimate radiation of the first wavelength towards the far field, said light source further comprising a second lens located adjacent to the second portion to collimate radiation of the second wavelength towards the far field.

27. The light source of claim 1, said periodic structure having a thickness not less than one wavelength of the radiation.

28. A light source for providing light, comprising:

a light emitting layer; and

a lens comprising a second layer in close proximity to the light emitting layer and with a periodic structure therein that is periodic along at least one direction in a plane, said structure comprising at least two optically transparent materials of different optical indices, one of said at least two optically transparent materials forming an array of scattering centers arranged in a regular pattern in the second layer, wherein the radiation propagating from the light emitting layer within an angle to a line normal to the plane will be transmitted by the second layer to a far field in an index-guided mode, and near field radiation propagating from the light emitting layer towards the second layer not within said angle to the line will be scattered and redirected by the array of scattering centers in the lens to the far field to thereby collimate the radiation propagating from the light emitting layer to the far field, wherein a collective interference light pattern is formed in the far field by said near field radiation, said pattern created by scattering from the array of scattering centers.

31. The light source of claim 28, wherein the periodic structure is optimized for collectively scattering light of a specific wavelength or wavelength range.

32. The light source of claim 28, wherein one of said at least two optically transparent materials forms an array of holes through the second layer or pillars in the second layer.

29. A method for collimating light to a far field, comprising:

providing a first layer with a periodic structure therein that is periodic along at least one direction in a plane, said structure comprising at least two optically transparent materials of different optical indices, one of said at least two optically transparent materials forming an array of scattering centers arranged in a regular pattern in the first layer; and

propagating radiation towards the first layer from a light source in close proximity to the first layer, so that the radiation propagating within an angle to a line normal to the plane towards the first layer will be transmitted by the first layer to the far field in an index-guided mode, and near field radiation propagating not within said angle to the line towards the first layer will be scattered and redirected by the array of scattering centers in the first layer to the far field to thereby collimate the near field radiation to the far field, said near field radiation forming in the far field a collective interference light pattern.

30. The method of claim 29, wherein the radiation propagating towards the first layer passes through a second layer before reaching the first layer.