TUNABLE LIQUID LENS WITH REDUCED ABERRATION

• US 20090213321A1
• Filed: 02/25/2009
• Published: 08/27/2009
• Est. Priority Date: 02/25/2008
• Status: Active Grant

• Current Assignee: Point Financial, Inc.
• Original Assignee: LensVector, Inc.
• Inventors: BAGRAMYAN, Aram, ASATRYAN, Karen, GALSTIAN, Tigran, PRESNIAKOV, Vladimir, TORK, Amir, ZOHRABYAN, Armen
• Granted Patent: US 8,072,574 B2
• Time in Patent Office: Days
• US Class Current: 349/200
• CPC Class Codes: G02B 3/14 of variable focal length
• CPC Class Codes: G02F 1/291 Two-dimensional analogue deflection
• CPC Class Codes: G03B 17/00 Details of cameras or camera bodies; Accessories therefor lens hoods or caps G03B11/04

Abstract

A tunable optical imaging system uses a fixed lens and a tunable liquid crystal lens that is operated only outside of an operational range of high aberration. A voltage range applied to change the optical power of the liquid crystal lens is limited to a continuous tunable range of low aberration. The relative positioning between the lens and a corresponding photodetector, and the relative lens powers of a fixed lens and the tunable lens, may be selected to compensate for any optical power offsets resulting from the limitation of the voltage range of the tunable lens. The lens may be operated in either positive tunability or negative tunability mode.

Claims

1. An imaging device comprising:

an image sensor;

a fixed lens assembly having a mounting for said image sensor at which a far field is in focus on said image sensor;

a tunable liquid crystal lens mounted in an optical path of said image sensor and said fixed lens assembly, said tunable liquid crystal lens having an optical power that increases from zero field level to a maximum power at a second field level, and decreases from said second field level to a non-zero end optical power at a desired maximum field level; and

an optical power adjustment element comprising at least one of a spacer and an additional lens, wherein said optical power adjustment element cancels said non-zero optical power so that said image sensor receives a far field image at said desired maximum field level.

2. The imaging device according to claim 1, wherein an initial optical power at zero field level is zero.

3. The imaging device according to claim 2, wherein said tunable liquid crystal lens comprises a flat liquid crystal layer and an electric field source providing a variable, spatially non-uniform electric field across the liquid crystal layer to provide a tunable range of optical power.

4. The imaging device according to claim 3, wherein said electric field source provides said additional lens.

5. The imaging device according to claim 1, wherein said source comprises an electric field controller setting an electric field control signal in response to a desired optical value signal, said electric field controller having an offset value restricting said tunable range to reduce an effect of at least one of aberration or scattering caused by said liquid crystal layer under conditions of lower or moderate electric fields.

6. The imaging device according to claim 5, further comprising an autofocus module that signals said controller to sweep said control signal from close focus near said second field level to far field focus near at said desired maximum focus until a focus position is found.

13. The imaging device according to claim 1, wherein said third field level results in an optical power of said layer that is, in absolute measurement, at least 5% less than said peak optical power when measured with respect to said initial optical power.

7. An imaging device comprising:

an image sensor;

a liquid crystal layer;

an electric field source providing a variable, spatially non-uniform electric field across the liquid crystal layer to provide a tunable range of optical power, wherein said layer, under the effect of said electric field, forms a tunable liquid crystal lens having a variable optical power that changes in a first direction with an increase in the strength of the electric field from an initial optical power to a peak optical power, and which changes in a second direction with a further increase of the strength of the electric field from said peak optical power to a non-zero end optical power different from the initial optical power, and wherein operation of the liquid crystal layer is limited to a continuous, non-zero tunable operational optical power range between the peak optical power and the end optical power; and

one or more fixed lenses cooperating with said liquid crystal lens at non-zero optical power to focus an image onto said image sensor with an infinity focus near one limit of said tunable range.

8. The imaging device according to claim 7, wherein said operational optical power range begins after a significant drop in optical aberration.

9. The imaging device according to claim 7, wherein said operational optical power range begins after a significant drop in optical scattering.

10. The imaging device according to claim 9, wherein said third field level results in an optical power of said layer that is, in absolute measurement, at least 10% less than said peak optical power when measured with respect to said initial optical power.

11. The imaging device according to claim 7, wherein said operational optical power range begins after a significant drop in both optical aberration and optical scattering.

12. The imaging device according to claim 7, wherein said liquid crystal layer is flat.

14. A method of controlling a tunable optical device having a liquid crystal layer and a variable, spatially non-uniform electric field applied across the liquid crystal layer to provide a tunable range of an optical property, the method comprising:

detecting at least one of aberration and scattering caused by said liquid crystal layer under conditions of relatively low electric fields and determining a corresponding optical quality of said device as a function of electric field;

determining a preferred range of operation for said electric field that avoids a range at which said optical quality is less desirable; and

generating said electric field in accordance with a desired optical value for said device within said preferred range of operation.

15. The method according to claim 14, wherein said device is a lens, said layer has a zero optical power at zero electric field, and said preferred range is at an electric field level above peak optical power and ending at a non-zero optical power at a desired maximum electric field.

16. The method according to claim 15, wherein said range is chosen such that an absolute upper limit optical power of said suitable range is at least 5% less than said peak optical power.

17. The method according to claim 15, wherein said range is chosen such that an absolute upper limit optical power of said suitable range is at least 10% less than said peak optical power.

18. The method according to claim 15, wherein said range is chosen taking into consideration optical aberration due to non-linearity in liquid crystal response to field level.

19. The method according to claim 15, wherein said range is chosen taking into consideration optical scattering.

20. The method according to claim 15, wherein said range is chosen taking into consideration optical scattering and optical aberration due to non-linearity in liquid crystal response to field level.

21. A tunable optical device having a liquid crystal layer and a variable, spatially non-uniform electric field applied across the liquid crystal layer to provide a tunable range of an optical property, said device having an electric field controller setting an electric field control signal in response to a desired optical value signal, said electric field controller having an offset value restricting a range of operation of said tunable range to reduce an effect of at least one of aberration and scattering caused by said liquid crystal layer under conditions of relatively low electric fields.

22. The tunable optical device according to claim 21, wherein said range begins after a significant drop in optical aberration.

23. The tunable optical device according to claim 21, wherein said range begins after a significant drop in optical scattering.

24. The tunable optical device according to claim 21, wherein said portion begins after a significant drop in both optical aberration and optical scattering.