Polarization-independent switchable lens system

• US 10,274,805 B2
• Filed: 06/13/2017
• Issued: 04/30/2019
• Est. Priority Date: 06/13/2017
• Status: Active Grant

• Current Assignee: Beam Engineering For Advanced Measurements Co.
• Original Assignee: Beam Engineering For Advanced Measurements Co.
• Inventors: Tabirian, Nelson V., Roberts, David E.
• Primary Examiner(s): Allen, Stephone B
• Assistant Examiner(s): Fissel, Travis S
• Application Number:
  US15/621,553
• Publication Number:
  US 20180356704A1
• Time in Patent Office: 686 Days
• Field of Search: 35115901, 35115903, 35115905, 35115939, 3511594, 35115955, 35115973, 35115975, 35115976, 351178
• CPC Class Codes: A61F 2/1627 for changing index of refraction, e.g. by external means or by tilting
• CPC Class Codes: A61F 2/1635 for changing shape
• CPC Class Codes: G02C 7/041 bifocal; multifocal
• CPC Class Codes: G02C 7/083 Electrooptic lenses
• CPC Class Codes: G02F 1/29 for the control of the position or the direction of light beams, i.e. deflection
• CPC Class Codes: G02F 2202/40 Materials having a particular birefringence, retardation
• CPC Class Codes: G02F 2203/06 Polarisation independent

Abstract

Energized lens systems and methods of fabricating an energized lens system which can be switched from one polarization-independent focal length to another polarization-independent focal length. The energized lens system can include a 90 degree twisted nematic liquid crystal layer with curved boundaries, and with transparent conductive electrodes which allow the application of an electric field to switch the focal length of the twisted nematic liquid crystal layer. The focal length of the energized lens system can be independent of the polarization of light in both of its two states, and only one liquid crystal layer of the energized lens system needs to be switched in order for the focal length of the energized lens system to be switched.

Claims

1. A polarizer-free single chamber energized lens system comprising:

a front optical system having at least a static refractive layer with a curved front surface and a curved back surface, and a focal length that is different for two polarizations of light;

a twisted nematic liquid crystal layer having at least a front curved surface, a back curved surface, and a nematic liquid crystal between the front curved surface and the back curved surface;

the front curved surface having at least a transparent conductive electrode and an alignment layer for aligning a portion of the liquid crystal adjacent to the alignment layer;

the back curved surface having at least a transparent conductive electrode and an alignment layer for aligning a portion of the liquid crystal adjacent to the alignment layer of the back curved surface, the alignment layer of the back curved surface oriented perpendicular to the alignment layer of the front curved surface;

the front curved surface and the back curved surface having different radii of curvature;

a thickness of a liquid crystal layer passing light therethrough meeting a Mauguin condition;

a back optical system having at least a static refractive layer with a curved front surface and a curved back surface, and a focal length that is different for two polarizations of light; and

a controller located outside an optical zone that enables application of an electric field between the transparent conductive electrodes of the twisted nematic liquid crystal layer, wherein the energized lens system is configured such that a focal length is different when an electric field is applied between the transparent conductive electrodes than when no such electric field is applied, and the focal length of the energized lens system is independent of the polarization of light whether or not an electric field is applied between the transparent conductive electrodes, wherein a single focal length is achieved with a single switchable liquid crystal layer, without a polarizer.

2. The energized lens system of claim 1 wherein the front optical system comprises a diffractive waveplate coating having lensing properties and a coating for conversion of circularly polarized light to linearly polarized light, and the back optical system comprises a coating for conversion of linearly polarized light to circularly polarized light and another diffractive waveplate coating having lensing properties.

3. The energized lens system of claim 1, wherein the energized lens system is configured as an ophthalmic lens device.

4. The energized lens system of claim 2, wherein the energized lens system is configured as an ophthalmic lens device.

5. The energized lens system of claim 1, wherein the energized lens system is configured as a contact lens.

6. The energized lens system of claim 2, wherein the energized lens system is configured as a contact lens.

7. The energized lens system of claim 1, wherein the energized lens system is configured as an intraocular lens.

8. The energized lens system of claim 2, wherein the energized lens system is configured as an intraocular lens.

9. The energized lens system of claim 1, wherein the energized lens system is configured as a spectacle lens.

10. The energized lens system of claim 2, wherein the energized lens system is configured as a spectacle lens.

11. The energized lens system of claim 1, wherein the Mauguin condition, includes:

d>

>

λ

/2Δ

n where, λ

is a wavelength of the light transmitted through the layer,

Δ

n is birefringence of the liquid crystal filling the space between two boundary surfaces of the layer, and radii of curvature of the two boundary surfaces are different so that a layer produces a focusing or defocusing effect, and thickness d of the layer varies with transverse position.

12. The energized lens system of claim 1, wherein the Mauguin condition is met at all transverse positions of the layer through which light is transmitted, and at all wavelengths within an operating wavelength band of the layer.

13. The energized lens system of claim 1 wherein the front optical system comprises a birefringent crystal with curved bounding surfaces, and the back optical system comprises a birefringent crystal with curved bounding surfaces.