Varying refractive index optical medium using at least two materials with thicknesses less than a wavelength

• US 7,426,328 B2
• Filed: 08/28/2003
• Issued: 09/16/2008
• Est. Priority Date: 08/28/2002
• Status: Expired due to Term

• Current Assignee: Seng-Tiong Ho
• Original Assignee: Phosistor Technologies
• Inventors: Zhou, Yan, Ho, Seng-Tiong
• Primary Examiner(s): Font; Frank G
• Assistant Examiner(s): CHIEM, DINH D
• Application Number:
  US10/652,269
• Publication Number:
  US 20050036738A1
• Time in Patent Office: 1,846 Days
• Field of Search: 385/33, 385/34, 385/124, 359652-654
• US Class Current: 385/124
• CPC Class Codes: G02B 6/32 having lens focusing means positioned between opposed fibre ends with lens being an integral part of the single fibre end G02B6/262

Abstract

An optical medium has a graded effective refractive index with a high maximum refractive index change. The medium is formed using alternating layers of two or more materials having significantly different refractive indices. The thickness of the layers of at least one of the materials is substantially less than the effective light wavelength of interest. The effective index of refraction in a local region within the medium depends on the ratio of the average volumes of the two materials in the local region. A graded index of refraction is provided by varying the relative thicknesses of the two materials.

Claims

1. A light transforming device having a graded index of refraction, comprising:

a body made substantially of a first amorphous material,

the body having embedded therein a plurality of discrete structures comprising a second amorphous material, each of the discrete structures having a size in at least one dimension substantially smaller than an effective wavelength of light in the second material,

wherein the first material has a first index of refraction and the second material has a second index of refraction different from the first index of refraction by at least Δ

n=0.5, and

wherein the size of the discrete structures in the at least one dimension is different in a first local region of the body than in a second local region of the body, thereby providing a graded index of refraction.

2. The light transforming device of claim 1, wherein the discrete structures include grains having a size in three dimensions that is substantially smaller than an effective wavelength of light in the second material.

3. A light transforming device having a graded index of refraction, comprising:

a plurality of alternating layers of a first amorphous material having a thickness and a second amorphous material, each layer of the second material having a thickness substantially less than an effective wavelength of light in the second material,

the first material having a first index of refraction,

the second material having a second index of refraction different from the first index of refraction by at least Δ

n=0.5,

the plurality of alternating layers forming a light transforming medium with an effective index of refraction in a local region that depends on a local ratio of a volume of the layers of the first material to a volume of the layers of the second material,

wherein a graded effective index of refraction along a direction transverse to the layers is formed by varying the thicknesses of the layers.

4. The light transforming device of claim 3, wherein the thickness of each layer of the second material is less than one-tenth the effective wavelength of light in the second material.

5. The light transforming device of claim 3, wherein each layer of the first material has a thickness substantially less than an effective wavelength of light in the first material.

6. The light transforming device of claim 5, wherein the thickness of each layer of the first material is less than one-tenth the effective wavelength of light in the first material.

7. The light transforming device of claim 3, wherein the thickness of each layer is controlled to within 0.5 nm and the effective index of refraction is controlled to within 0.005.

8. The light transforming device of claim 3, wherein at least one of the first material and the second material is an amorphous material.

9. The light transforming device of claim 8, wherein the first material comprises silicon dioxide and the second material comprises tantalum pentoxide.

10. The light transforming device of claim 8, wherein the first material comprises silicon dioxide and the second material comprises titanium dioxide.

11. The light transforming device of claim 3, wherein the first material comprises silicon dioxide and the second material comprises silicon.

12. The light transforming device of claim 3, wherein at least one of the first material and the second material is a polycrystalline material.

13. The light transforming device of claim 3, wherein the layers are substantially planar.

14. The light transforming device of claim 3, wherein the graded effective index of refraction is a parabolic function of position along the direction transverse to the layers.

15. The light transforming device of claim 3, wherein the device has a length such that light having a large mode size entering at a first end of the device and propagating longitudinally through the device is focused to a small mode size at a second end of the device.

16. The light transforming device of claim 15, wherein the small mode size is less than 1 μ

m.

17. The light transforming device of claim 3, wherein the device has a length such that light having a large mode size entering at a first end of the device and propagating longitudinally through the device is focused to a small mode size at a focal point outside a second end of the device.

18. The light transforming device of claim 3, wherein the small mode size is less than 1 μ

m.

19. The light transforming device of claim 3, wherein the effective index of refraction varies such that a mode profile of light propagating through the device is transformed from a first mode profile substantially matching a mode profile for light propagating in a single mode fiber to a second mode profile substantially matching a mode profile for light propagating in a semiconductor waveguide.

20. A light transforming device having a graded index of refraction, comprising:

a plurality of alternating layers of a first amorphous material having a thickness and a second amorphous material, each layer of the second material having a thickness substantially less than an effective wavelength of light in the second material,

the first material having a first index of refraction,

the second material having a second index of refraction different from the first index of refraction,

the plurality of alternating layers forming a light transforming medium with an effective index of refraction in a local region that depends on a local ratio of a volume of the layers of the first amorphous material to a volume of the layers of the second amorphous material, wherein a graded effective index of refraction along a direction transverse to the layers is formed by varying the thicknesses of the layers.

21. The light transforming device of claim 20, wherein the thickness of each layer of the second material is less than one tenth the effective wavelength of light in the second material.

22. The light y transforming device of claim 20, wherein the thickness of each layer is less than one-tenth the effective wavelength of light in the respective material.

23. The light transforming device of claim 20, wherein the second index of refraction is different from the first index of refraction by at least 0.2.

24. The light transforming device of claim 20, wherein the thickness of each layer is controlled to within 0.5 nm and the effective index of refraction is controlled to within 0.005.

25. The light transforming device of claim 20, wherein the first material comprises silicon dioxide and the second material comprises titanium dioxide.

26. The light transforming device of claim 20, wherein the first material comprises silicon dioxide and the second material comprises silicon.

27. The light transforming device of claim 20, wherein the first material comprises silicon dioxide and the second material comprises tantalum pentoxide.

28. The light transforming device of claim 20, wherein the layers are substantially planar.

29. The light transforming device of claim 20, wherein the graded effective index of refraction is a parabolic function of position along the direction transverse to the layers.

30. The light transforming device of claim 20, wherein the device has a length such that light having a large mode size entering at a first end of the device and propagating longitudinally through the device is focused to a small mode size at a second end of the device.

31. The light transforming device of claim 30, wherein the device has a length such that light having a large mode size entering at a first end of the device and propagating longitudinally through the device is focused to a small mode size at a focal point outside a second end of the device.

32. The light transforming device of claim 30, wherein the small mode size is less than 1 μ

m.

33. The light transforming device of claim 20, wherein the effective index of refraction varies such that a mode profile of light propagating through the device is transformed from a first mode profile substantially matching a mode profile for light propagating in a single mode fiber to a second mode profile substantially matching a mode profile for light propagating in a semiconductor waveguide.