Method and apparatus for adjusting the focal length of a optical system

• US 5,091,801 A
• Filed: 10/19/1989
• Issued: 02/25/1992
• Est. Priority Date: 10/19/1989
• Status: Expired due to Fees

• Current Assignee: North East Research Associates Incorporated
• Original Assignee: North East Research Associates Incorporated
• Inventors: Ebstein, Steven
• Primary Examiner(s): Arnold, Bruce Y.
• Assistant Examiner(s): Gass, Rebecca D.
• Application Number:
  US07/424,190
• Time in Patent Office: 859 Days
• Field of Search: 350/418, 350/419, 350/442
• US Class Current: 359/665
• CPC Class Codes: G02B 3/12 Fluid-filled or evacuated lenses
• CPC Class Codes: G02F 1/29 for the control of the position or the direction of light beams, i.e. deflection

Abstract

A nearly index matched (NIM) optic is formed from at least two elements having indices of refraction that are substantially the same over a given range of wavelengths. The optical cell can have matched solid and fluid lenses in which the solid has at least one curved interface in contact with the fluid. The solid and fluid share a boundary with equal but opposite curvature at each point over the aperture of the NIM optic. The effective optical curvature of the boundary is reduced by the difference in the index of refraction between the two elements of the NIM optic. This difference in the index of refraction can be controlled by changing the index of refraction of at least one of the elements so as to change the difference in the index of refraction across the optical boundary.

Claims

1. A nearly index matched (NIM) optic, comprising:

means for receiving light from a light source, the light having a given range of wavelengths;

means for transferring the light across at least a first surface into a first material having a first index of refraction;

means for refracting the light across at least a first boundary formed in the first material, each point on the first boundary having an optical curvature of a given sign; and

means for refracting the light at a second boundary formed in a second material that has a second index of refraction, each point on the second boundary corresponding to a point on the first boundary, each point on the second boundary having an optical curvature that is equal to the curvature of the corresponding point on the first boundary but opposite in sign, said first and second indices selected such that a difference between the second index of refraction and the first index of refraction is less than 0.1 and substantially the same over the range of wavelengths of the light, whereby the absolute value of the optical curvature at corresponding points on the first and second boundaries is reduced by the absolute value of the difference between the first and second indices of refraction thereby permitting control of focal length through selection of said indices.

2. An optical system as claimed in claim 1, wherein the light source is monochromatic.

3. An optical system as claimed in claim 2, wherein the light source is a laser.

4. An optical system as claimed in claim 1, wherein the first surface is flat.

5. An optical system as claimed in claim 1, wherein:

the first boundary contacts the second boundary; and

the second material is a fluid when it first contacts the first material.

6. An optical system as claimed in claim 5, further comprising means for changing the second index of refraction of the second material.

7. An optical system as claimed in claim 1, wherein the second material further comprises a second surface.

8. An optical system as claimed in claim 7, further comprising means for reflecting the light off a second surface of the second material that is positioned opposite the second boundary.

9. A lens, comprising:

a first element having a first surface and at least a first optical boundary, every point on the first optical boundary having a first optical curvature of a given sign, the first element being made from a first material having a first index of refraction, for a predetermined wavelength range of light; and

a second element having at least a second optical boundary, each point on the second optical boundary corresponding to a point on the first optical boundary, each point on the second optical boundary having a second optical curvature that is equal to the first optical curvature of the corresponding point on the first optical boundary but opposite in sign, the second element being made from a second material having a second index of refraction, said first and second indices selected such that a difference formed by subtracting the first and second indices of refraction is less than 0.1 and substantially the same for the wavelength range of light, whereby the absolute value of the first and second optical curvatures is reduced by the absolute magnitude of the difference between the first and second indices of refraction, thereby permitting control of focal length through selection of said indices.

10. A lens as claimed in claim 9, wherein the first and second elements contact each other.

11. A lens as claimed in claim 10, wherein the second material is a fluid.

12. A lens as claimed in claim 9, further comprising means for changing the index of refraction of the fluid at the wavelength of the light.

13. A lens as claimed in claim 9, wherein the means for changing the index of refraction is chosen from the group consisting of:

(a) an electro-optical connection that changes the index of refraction of the fluid at the wavelength of the light electronically;

(b) a magneto-optical connection that changes the index of refraction of at least the fluid at the wavelength of the light magnetically;

(c) a thermal connection that changes the index of refraction of at least the fluid by changing its temperature;

(d) a pump connection that changes the index of refraction of at least the fluid by changing the second material comprising the second lens; and

(e) a pressure vessel that changes the index of refraction of at least the fluid using pressure.

14. A lens as claimed in claim 13, wherein the first and second surfaces of the first are optically flat.

15. A lens as claimed in claim 13, wherein the light is monochromatic.

16. A lens as claimed in claim 15, wherein the light source is a laser.

17. A method for obtaining a very small change in the focal length in an optical system, comprising the steps of:

receiving light from a light source, the light having a given range of wavelengths;

transferring the light across a first surface into a first material having a first index of refraction;

refracting the light at a first optical boundary of the first material, every point on the first optical boundary having a curvature of a given sign; and

reducing the absolute value of the curvature of each point on the first optical boundary by refracting light from each point on the first optical boundary at a corresponding point on a second boundary made from a second material that has a second index of refraction, the second optical boundary having a second optical curvature that is equal in magnitude to the curvature of the first optical boundary but that has a second sign that is opposite the first sign, and selecting said first and second indices such that a difference formed by subtracting the first index of refraction and the second index of refraction is less than 0.1 and substantially the same over the range of wavelengths of the light, whereby the absolute value of each point on the first optical boundary is reduced by the difference between the first index of refraction and the second index of refraction.

18. A method as claimed in claim 17, wherein the light is monochromatic.

19. A method as claimed in claim 18, wherein the monochromatic light is generated by a laser.

20. A method as claimed in claim 17, further comprising the step of changing the second index of refraction of the second material.

21. A method as claimed in claim 17, further comprising the step of reflecting the light off a second optically flat surface of the second material that is positioned opposite the second curved surface.